Updated on 2024/12/13

写真a

 
OHTSUBO Takashi
 
Organization
Academic Assembly Institute of Science and Technology Fundamental Sciences Associate Professor
Graduate School of Science and Technology Fundamental Sciences Associate Professor
Faculty of Science Department of Science Associate Professor
Title
Associate Professor
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Degree

  • 博士(理学) ( 1994.6   大阪大学 )

Research Interests

  • Nuclear electro nagnetic moments

  • 超微細構造相互作用

  • 原子核の電磁気モーメント

  • Hyperfine Interaction

Research Areas

  • Natural Science / Magnetism, superconductivity and strongly correlated systems

  • Natural Science / Semiconductors, optical properties of condensed matter and atomic physics

  • Natural Science / Theoretical studies related to particle-, nuclear-, cosmic ray and astro-physics

Research History (researchmap)

  • Niigata University   Department of Physics, Faculty of Science   Associate Professor

    2007.4

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  • Niigata University   Department of Physics, Faculty of Science   Associate Professor (as old post name)

    2004.4 - 2007.3

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  • 文部省在外研究員(ドイツ)

    1999 - 2000

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  • Monbusho-sponsored Japanese Ouerseas Research Fellow

    1999 - 2000

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  • - 新潟大学理学部 助手

    1994.4 - 2004.3

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  • - Research Associate, Faculty of Science, Niigata University

    1994

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Research History

  • Niigata University   Faculty of Science Department of Science   Associate Professor

    2017.4

  • Niigata University   Graduate School of Science and Technology Fundamental Sciences   Associate Professor

    2010.4

  • Niigata University   Graduate School of Science and Technology Fundamental Sciences   Associate Professor

    2010.4

  • Niigata University   Faculty of Science Department of Physics   Associate Professor

    2004.4 - 2017.3

  • Niigata University   Faculty of Science Department of Physics   Assistant Professor

    1994.4 - 2004.3

Education

  • Osaka University   Graduate School, Division of Natural Science   Physics

    - 1994

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  • Osaka University   理学研究科   物理学

    - 1994

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    Country: Japan

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  • Osaka University   Faculty of Science   Physics

    - 1988

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  • Osaka University   School of Science   物理

    - 1988

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    Country: Japan

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Professional Memberships

 

Papers

  • The on-line low temperature nuclear orientation facility NICOLE Reviewed

    T. Ohtsubo, S. Roccia, N. J. Stone, J. R. Stone, C. Gaulard, U. Koester, J. Nikolov, G. S. Simpson, M. Veskovic

    JOURNAL OF PHYSICS G-NUCLEAR AND PARTICLE PHYSICS   44 ( 4 )   2017.4

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    Language:English   Publishing type:Research paper (scientific journal)   Publisher:IOP PUBLISHING LTD  

    We review major experiments and results obtained by the on-line low temperature nuclear orientation method at the NICOLE facility at ISOLDE, CERN since the year 2000 and highlight their general physical impact. This versatile facility, providing a large degree of controlled nuclear polarization, was used for a long-standing study of magnetic moments at shell closures in the region Z - 28, N - 28-50 but also for dedicated studies in the deformed region around A similar to 180. Another physics program was conducted to test symmetry in the weak sector and constrain weak coupling beyond V-A. Those two programs were supported by careful measurements of the involved solid state physics parameters to attain the full sensitivity of the technique and provide interesting interdisciplinary results. Future plans for this facility include the challenging idea of measuring the beta-gamma-neutron angular distributions from polarized beta delayed neutron emitters, further test of fundamental symmetries and obtaining nuclear structure data used in medical applications. The facility will also continue to contribute to both the nuclear structure and fundamental symmetry test programs.

    DOI: 10.1088/1361-6471/aa5f22

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  • DEVELOPMENT OF HIGH RESOLUTION TOF DETECTOR FOR RI BEAMS USING CHERENKOV RADIATION Reviewed

    E. Miyata, M. Takechi, T. Ohtsubo, M. Fukuda, D. Nishimura, K. Abe, K. Aoki, A. Ikeda, T. Izumikawa, H. Oikawa, K. Ohnishi, S. Ohmika, I. Kato, Y. Kanke, N. Kanda, R. Kanbe, H. Kikuchi, A. Kitagawa, S. Sato, H. Shimamura, J. Shimaya, S. Suzuki, T. Suzuki, R. Takagaki, H. Takahashi, Y. Takei, Y. Takeuchi, T. Takenouchi, N. Tadano, M. Tanaka, Y. Tanaka, K. Chikaato, H. Du, J. Nagumo, K. Nishizuka, T. Nishimura, S. Fukuda, M. Machida, A. Mizukami, M. Mihara, J. Muraoka, S. Yagi, S. Yamaoka, T. Yamaguchi, K. Yokoyama

    ACTA PHYSICA POLONICA B   48 ( 3 )   409 - 414   2017.3

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    Language:English   Publishing type:Research paper (scientific journal)   Publisher:JAGIELLONIAN UNIV PRESS  

    We have developed a high time resolution time-of-flight (TOF) detector that detects the Cherenkov light emitted when an RI beam passes through a high refractive index glass. Ni-58 and Xe-132 beams of energies of 200 A 500 A MeV and secondary beams produced with those beams have been used for the test of the Cherenkov detectors. The time resolution of sigma = 5 ps with the inclusion of system resolution has been achieved with a 420 A MeV Xe-132 beam.

    DOI: 10.5506/APhysPolB.48.409

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  • NUCLEAR STRUCTURE OF C-15,C-16 VIA REACTION CROSS-SECTION MEASUREMENTS Reviewed

    H. Du, M. Fukuda, D. Nishimura, M. Takechi, T. Suzuki, Y. Tanaka, I. Kato, M. Tanaka, K. Abe, T. Izumikawa, H. Oikawa, T. Ohtsubo, J. Ohno, Y. Kanke, H. Kikuchi, A. Kitagawa, S. Sato, U. Sayama, J. Shimaya, S. Suzuki, Y. Takeuchi, T. Takemoto, N. Tadano, R. Tamura, J. Nagumo, K. Nishizuka, S. Fukuda, K. Hori, S. Matsunaga, A. Mizukami, M. Mihara, E. Miyata, D. Murooka, S. Yamaoka, T. Yamaguchi

    ACTA PHYSICA POLONICA B   48 ( 3 )   473 - 479   2017.3

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    Language:English   Publishing type:Research paper (scientific journal)   Publisher:JAGIELLONIAN UNIV PRESS  

    Reaction cross sections for C-15.16 on nuclear targets (Be, C, Al) and proton target are systematically measured in the intermediate energy range. Nucleon density distributions of C-15,C-16 were deduced from the analyses of present data with existing experimental data using the Glauber-type calculation. Proton and neutron density distributions were also deduced separately from proton target data. Results of root-mean-square radii show a good agreement with theoretical calculations for both isotopes.

    DOI: 10.5506/APhysPolB.48.473

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  • REACTION CROSS SECTIONS FOR B13-15 AND ONE-NEUTRON HALO IN B-14 Reviewed

    M. Tanaka, M. Fukuda, D. Nishimura, M. Takechi, S. Suzuki, H. Du, Y. Tanaka, K. Aoki, S. Fukuda, A. Honma, T. Izumikawa, Y. Kamisho, N. Kanda, I. Kato, Y. Kanke, A. Kitagawa, J. Kohno, M. Machida, K. Matsuta, M. Mihara, E. Miyata, Y. Morita, J. Muraoka, D. Murooka, T. Nagai, M. Nagashima, K. Ohnishi, J. Ohno, T. Ohtsubo, H. Oikawa, S. Sato, H. Shimamura, T. Sugihara, T. Suzuki, N. Tadano, R. Takagaki, Y. Takei, A. Takenouchi, S. Yagi, T. Yamaguchi, S. Yamaki, S. Yamaoka

    ACTA PHYSICA POLONICA B   48 ( 3 )   461 - 466   2017.3

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    Language:English   Publishing type:Research paper (scientific journal)   Publisher:JAGIELLONIAN UNIV PRESS  

    We have measured reaction cross sections (sigma(R)) for B-13,B-14,B-15 on Be, C, Al, and proton targets. In addition to the conventional method of deducing nucleon density distributions based on the Glauber-type calculation, the recently developed method for deducing point- proton and neutron density distributions separately from sigma(R) on proton targets were utilized for these nuclei. The result suggests the necessity for B-14 of a large tail in its neutron density distribution, which can be referred to as a one-neutron halo. Root-mean-square point- proton, neutron and matter radii for B-13,B-14,B-15 were also derived. From present systematic studies for B-13,B-14,B-15, a large enhancement of matter and neutron radii in B-14 was found for the first time.

    DOI: 10.5506/APhysPolB.48.461

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  • New results from isochronous mass measurements of neutron-rich uranium fission fragments with the FRS-ESR-facility at GSI Reviewed

    R. Knoebel, M. Diwisch, H. Geissel, Yu. A. Litvinov, Z. Patyk, W. R. Plass, C. Scheidenberger, B. Sun, H. Weick, F. Bosch, D. Boutin, L. Chen, C. Dimopoulou, A. Dolinskii, B. Franczak, B. Franzke, M. Hausmann, C. Kozhuharov, J. Kurcewicz, S. A. Litvinov, M. Matos, M. Mazzocco, G. Muenzenberg, S. Nakajima, C. Nociforo, F. Nolden, T. Ohtsubo, A. Ozawa, J. Stadlmann, M. Steck, T. Suzuki, P. M. Walker, M. Winkler, T. Yamaguchi

    EUROPEAN PHYSICAL JOURNAL A   52 ( 5 )   2016.5

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    Language:English   Publishing type:Research paper (scientific journal)   Publisher:SPRINGER  

    Masses of uranium fission fragments have been measured with the FRagment Separator (FRS) combined with the Experimental Storage Ring (ESR) at GSI. A 410-415MeV/u U-238 projectile beam was fast extracted from the synchrotron SIS-18 with an average intensity of 10(9)/spill. The projectiles were focused on a 1 g/cm(2) beryllium target at the entrance of the FRS to create neutron-rich isotopes via abrasion-fission. The fission fragments were spatially separated with the FRS and injected into the isochronous storage ring ESR for fast mass measurements without applying cooling. The Isochronous Mass Spectrometry (IMS) was performed under two different experimental conditions, with and without B.-tagging at the high-resolution dispersive central focal plane of the FRS. The evaluation has been done for the combined data sets from both experiments with a new method of data analysis. The use of a correlation matrix has provided experimental mass values for 23 different neutron-rich isotopes for the first time and 6 masses with improved values. The new masses were obtained for nuclides in the element range from Se to Ce. The applied analysis has given access even to rare isotopes detected with an intensity of a few atoms per week. The novel data analysis and systematic error determination are described and the results are compared with extrapolations of experimental values and theoretical models.

    DOI: 10.1140/epja/i2016-16138-6

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  • First direct mass measurements of stored neutron-rich Cd-129,Cd-130,Cd-131 isotopes with FRS-ESR Reviewed

    R. Knoebel, M. Diwisch, F. Bosch, D. Boutin, L. Chen, C. Dimopoulou, A. Dolinskii, B. Franczak, B. Franzke, H. Geissel, M. Hausmann, C. Kozhuharov, J. Kurcewicz, S. A. Litvinov, G. Martinez-Pinedo, M. Matos, M. Mazzocco, G. Muenzenberg, S. Nakajima, C. Nociforo, F. Nolden, T. Ohtsubo, A. Ozawa, Z. Patyk, W. R. Plass, C. Scheidenberger, J. Stadlmann, M. Steck, B. Sun, T. Suzuki, P. M. Walker, H. Weick, M. -R. Wu, M. Winkler, T. Yamaguchi

    PHYSICS LETTERS B   754   288 - 293   2016.3

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    Language:English   Publishing type:Research paper (scientific journal)   Publisher:ELSEVIER SCIENCE BV  

    A 410 MeV/u U-238 projectile beam was used to create cadmium isotopes via abrasion-fission in a beryllium target placed at the entrance of the in-flight separator FRS at GSI. The fission fragments were separated by the FRS and injected into the isochronous storage ring ESR for mass measurements. Isochronous Mass Spectrometry (IMS) was performed under two different experimental conditions, with and without B rho-tagging at the high-resolution central focal plane of the FRS. In the experiment with B rho-tagging the magnetic rigidity of the injected fragments was determined with an accuracy of 2 . 10(-4). A new method of data analysis, which uses a correlation matrix for the combined data set from both experiments, has provided experimental mass values of 25 rare isotopes for the first time. The high sensitivity and selectivity of the method have given access to nuclides detected with a rate of a few atoms per week. In this letter we present for the Cd-129,Cd-130,Cd-131 isotopes mass values directly measured for the first time. The experimental mass values of cadmium as well as for tellurium and tin isotopes show a pronounced shell effect towards and at N=82. Shell quenching cannot be deduced from a single new mass value, nor by a better agreement with a theoretical model which explicitly takes into account a quenching feature. This is in agreement with the conclusion from gamma-ray spectroscopy and confirms modern shell-model calculations. (C) 2016 Published by Elsevier B.V. This is an open access article under the CC BY license.

    DOI: 10.1016/j.physletb.2016.01.039

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  • Between atomic and nuclear physics: radioactive decays of highly-charged ions Reviewed

    Dinko Atanasov, Klaus Blaum, Fritz Bosch, Carsten Brandau, Paul Buehler, Xiangcheng Chen, Iris Dillmann, Thomas Faestermann, Bingshui Gao, Hans Geissel, Roman Gernhaeuser, Siegbert Hagmann, Takuji Izumikawa, Pierre-Michel Hillenbrand, Christophor Kozhuharov, Jan Kurcewicz, Sergey A. Litvinov, Yuri A. Litvinov, Xinwen Ma, Gottfried Muenzenberg, Mohammad Ali Najafi, Fritz Nolden, Takashi Ohtsubo, Akira Ozawa, Fatma Cagla Ozturk, Zygmunt Patyk, Matthew Reed, Rene Reifarth, Mohammad Shahab Sanjari, Dieter Schneider, Markus Steck, Thomas Stoehlker, Baohua Sun, Fumi Suzaki, Takeshi Suzuki, Christian Trageser, Xiaolin Tu, Tomohiro Uesaka, Philip Walker, Meng Wang, Helmut Weick, Nicolas Winckler, Philip Woods, Hushan Xu, Takayuki Yamaguchi, Xinliang Yan, Yuhu Zhang

    JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS   48 ( 14 )   2015.7

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    Highly charged radioactive ions can be stored for extended periods of time in storage rings which allows for precision measurements of their decay modes. The straightforward motivation for performing such studies is that fully ionised nuclei or few-electron ions can be viewed as clean quantum-mechanical systems, in which the interactions of the many electrons can be either excluded or treated precisely. Thus, the influence of the electron shell on the decay probability can be investigated. Another important motivation is stellar nucleosynthesis, which proceeds at high temperatures and the involved atoms are therefore highly ionised. Presented here is a compact review of the relevant experiments conducted at heavy-ion storage rings. Furthermore, we outline the perspectives for future experiments at new-generation storage-ring facilities.

    DOI: 10.1088/0953-4075/48/14/144024

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  • beta-NMR study of boron in diamond Reviewed

    T. Izumikawa, M. Mihara, K. Matsuta, M. Fukuda, T. Ohtsubo, S. Ohya, T. Minamisono

    HYPERFINE INTERACTIONS   230 ( 1-3 )   11 - 14   2015.4

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    Language:English   Publishing type:Research paper (international conference proceedings)   Publisher:SPRINGER  

    A beta-NMR study of B-12 implanted in diamond was performed in order to investigate the implantation sites and the defects. The maintained polarization of B-12 was measured by use of widely modulated rf around the Larmor frequency (nu = nu (L) +/- 200 kHz) as a function of temperature from 160 K to 320 K. The observed polarization was found to be almost constant at about 0.9 % in this temperature range. The initial polarization for this system was obtained as about 8.1 %. Therefore about 10 % of the implanted B-12 maintained its polarization in this frequency range. Conversely, about 90 % of the implanted B-12 was undetected in the present experiment.

    DOI: 10.1007/s10751-014-1090-z

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  • Observation of muonic X-rays of cosmic-ray muons stopped in Al and Fe targets Reviewed

    Yoshihiro Shimbara, Teiichiro Matsuzaki, Kosuke Abe, Yoshitaka Fujita, Jun Goto, Takeshi Itoh, Naoki Kikukawa, Masayuki Nagashima, Yoshihiro Nakamura, Toshiyuki Ogura, Takashi Ohtsubo, Susumu Ohya, Taku Sakai, Daishiro Sera, Shinji Suzuki, Kosumo Takeda, Azumi Yajima, Takenori Yoshikawa

    Journal of the Physical Society of Japan   84 ( 3 )   2015.3

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    © 2015 The Physical Society of Japan. We successfully measured muonic X-rays of cosmic-ray muons stopped in Al and Fe targets. In order to identify the events that incoming cosmic-ray muons were stopped in the targets, a coincidence and anticoincidence system of three plastic scintillators was used. The X-rays associated with the atomic muon captures were measured with germanium detectors. Measurements using the Al and Fe targets were carried out for 33 and 16 days, respectively. A sufficient number of muonic X-ray events for identifying the elemental compositions of the target materials were clearly observed. This technique provides a means of nondestructive elemental analysis that does not require the use of particle accelerators.

    DOI: 10.7566/JPSJ.84.034301

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  • Density distribution of Li-8 and B-8 and capture reaction at low energy Reviewed

    G. W. Fan, M. Fukuda, D. Nishimura, X. L. Cai, S. Fukuda, I. Hachiuma, C. Ichikawa, T. Izumikawa, M. Kanazawa, A. Kitagawa, T. Kuboki, M. Lantz, M. Mihara, M. Nagashima, K. Namihira, Y. Ohkuma, T. Ohtsubo, Zhongzhou Ren, S. Sato, Z. Q. Sheng, M. Sugiyama, S. Suzuki, T. Suzuki, M. Takechi, T. Yamaguchi, W. Xu

    PHYSICAL REVIEW C   91 ( 1 )   2015.1

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    Language:English   Publishing type:Research paper (scientific journal)   Publisher:AMER PHYSICAL SOC  

    Reaction cross sections of Li-8 on stable targets were measured at intermediate energies. With the existing experimental data of interaction cross sections at 790 MeV/nucleon the nucleon density distribution of Li-8 was extracted by the use of the modified Glauber model. Meanwhile, the existing data of B-8 have been also reanalyzed. Structures of Li-8 and B-8 were compared through the density. On the basis of dilute surface densities, the discussion of Li-7(n,gamma) Li-8 and Be-7(p,gamma) B-8 capture reactions was performed within the framework of the direct capture reaction mechanism. The calculations agreed quite well with the experimental data as well as other analyses.

    DOI: 10.1103/PhysRevC.91.014614

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  • Evidence of halo structure in Mg-37 observed via reaction cross sections and intruder orbitals beyond the island of inversion Reviewed

    M. Takechi, S. Suzuki, D. Nishimura, M. Fukuda, T. Ohtsubo, M. Nagashima, T. Suzuki, T. Yamaguchi, A. Ozawa, T. Moriguchi, H. Ohishi, T. Sumikama, H. Geissel, N. Aoi, Rui-Jiu Chen, De-Qing Fang, N. Fukuda, S. Fukuoka, H. Furuki, N. Inabe, Y. Ishibashi, T. Itoh, T. Izumikawa, D. Kameda, T. Kubo, M. Lantz, C. S. Lee, Yu-Gang Ma, K. Matsuta, M. Mihara, S. Momota, D. Nagae, R. Nishikiori, T. Niwa, T. Ohnishi, K. Okumura, M. Ohtake, T. Ogura, H. Sakurai, K. Sato, Y. Shimbara, H. Suzuki, H. Takeda, S. Takeuchi, K. Tanaka, M. Tanaka, H. Uenishi, M. Winkler, Y. Yanagisawa, S. Watanabe, K. Minomo, S. Tagami, M. Shimada, M. Kimura, T. Matsumoto, Y. R. Shimizu, M. Yahiro

    PHYSICAL REVIEW C   90 ( 6 )   2014.12

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    Precise reaction cross sections (sigma R) for (24- 38) Mg on C targets at energies around 240 MeV/nucleon have been measured at the Radioactive Isotope Beam Factory at RIKEN. The sigma R for (36-38) Mg have been measured for the first time. An enhancement of sR compared to the systematics for spherical stable nuclei has been observed, especially in the neutron-rich region, which reflects the deformation of those isotopes. In the vicinity of the drip line the sR for Mg-37 is especially large. It is shown by analysis using a recently developed theoretical method that this prominent enhancement of sR for Mg-37 should come from the p-orbital halo formation breaking the N = 28 shell gap.

    DOI: 10.1103/PhysRevC.90.061305

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  • Structure of Li-8 from a reaction cross-section measurement Reviewed

    G. W. Fan, M. Fukuda, D. Nishimura, X. L. Cai, S. Fukuda, I. Hachiuma, C. Ichikawa, T. Izumikawa, M. Kanazawa, A. Kitagawa, T. Kuboki, M. Lantz, M. Mihara, M. Nagashima, K. Namihira, Y. Ohkuma, T. Ohtsubo, Zhongzhou Ren, S. Sato, Z. Q. Shen, M. Sugiyama, S. Suzuki, T. Suzuki, M. Takechi, T. Yamaguchi, B. J. Xu, W. Xu

    PHYSICAL REVIEW C   90 ( 4 )   2014.10

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    We have precisely measured reaction cross sections (sigma(R)) for Li-8 using Be-9, C-12, Al-27, and proton targets at intermediate energies by the transmission method. From the energy dependence of the sigma(R) including the high energy data, the density distribution of Li-8 was deduced through a modified Glauber model. It is shown that Li-8 has a shorter tail structure in the density as compared with that of B-8 and the matter radius of Li-8 is similar to those of the other nonhalo Li isotopes. The result is consistent with the previous experiments that there is a tendency for Li-8 to be a skin nucleus.

    DOI: 10.1103/PhysRevC.90.044321

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  • Density distribution of Be-14 from reaction cross-section measurements Reviewed

    T. Moriguchi, A. Ozawa, S. Ishimoto, Y. Abe, M. Fukuda, I. Hachiuma, Y. Ishibashi, Y. Ito, T. Kuboki, M. Lantz, D. Nagae, K. Namihira, D. Nishimura, T. Ohtsubo, H. Ooishi, T. Suda, H. Suzuki, T. Suzuki, M. Takechi, K. Tanaka, T. Yamaguchi

    NUCLEAR PHYSICS A   929   83 - 93   2014.9

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    We measured the reaction cross sections of the two-neutron halo nucleus Be-14 with proton and carbon targets at about 41 and 76 MeV/nucleon. Based on a Glauber model calculation, we deduced the matter density distribution of Be-14 in which previously measured interaction cross sections at relativistic energies were also included. An s-wave dominance in Be-14 has been confirmed, although the halo tail of Be-14 is not distributed as much as that of Li-11. Significant mixing of the p-wave in addition to the s- and d-wave is also suggested. (C) 2014 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nuclphysa.2014.06.003

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  • Magnetic properties of Hf-177 and Hf-180 in the strong-coupling deformed model Reviewed

    S. Muto, N. J. Stone, C. R. Bingham, J. R. Stone, P. M. Walker, G. Audi, C. Gaulard, U. Koester, J. Nikolov, K. Nishimura, T. Ohtsubo, Z. Podolyak, L. Risegari, G. S. Simpson, M. Veskovic, W. B. Walters

    PHYSICAL REVIEW C   89 ( 4 )   2014.4

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    This paper reports NMR measurements of the magnetic dipole moments of two high-K isomers, the 37/2(-), 51.4 m, 2740 keV state in Hf-177 and the 8(-), 5.5 h, 1142 keV state in Hf-180 by the method of on-line nuclear orientation. Also included are results on the angular distributions of. transitions in the decay of the 177Hf isotope. These yield high precision E2/M1 multipole mixing ratios for transitions in bands built on the 23/2(+), 1.1 s, isomer at 1315 keV and on the 9/2(+), 0.663 ns, isomer at 321 keV. The new results are discussed in the light of the recently reported finding of systematic dependence of the behavior of the g(R) parameter upon the quasiproton and quasineutron make up of high-K isomeric states in this region.

    DOI: 10.1103/PhysRevC.89.044309

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  • Charge-changing cross sections of Ne-30, Na-32,Na-33 with a proton target Reviewed

    A. Ozawa, T. Moriguchi, T. Ohtsubo, N. Aoi, D. Q. Fang, N. Fukuda, M. Fukuda, H. Geissel, I. Hachiuma, N. Inabe, Y. Ishibashi, S. Ishimoto, Y. Ito, T. Izumikawa, D. Kameda, T. Kubo, T. Kuboki, K. Kusaka, M. Lantz, Y. G. Ma, M. Mihara, Y. Miyashita, S. Momota, D. Nagae, K. Namihira, D. Nishimura, H. Ooishi, Y. Ohkuma, T. Ohnishi, M. Ohtake, K. Ogawa, Y. Shimbara, T. Suda, T. Sumikama, H. Suzuki, S. Suzuki, T. Suzuki, M. Takechi, H. Takeda, K. Tanaka, R. Watanabe, M. Winkler, T. Yamaguchi, Y. Yanagisawa, Y. Yasuda, K. Yoshinaga

    PHYSICAL REVIEW C   89 ( 4 )   2014.4

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    The total charge-changing, charge pick-up, and partial charge-changing cross sections of very neutron-rich nuclei (Ne-30, Na-32,Na-33) with a proton target have been measured at similar to 240A MeV for the first time. We introduced the phenomenological correction factor in Glauber-model calculations for the total charge-changing cross sections with the proton target, and applied it to deduce the proton radii of these nuclei. For 30Ne and Na-32, the neutron skin thicknesses of the nuclei were deduced by comparing the proton radii with the matter radii deduced from the interaction cross-section measurements. A significant thick neutron-skin has been observed for the nuclei. We also found that the charge pick-up cross sections are much larger than those in the systematics of stable nuclei.

    DOI: 10.1103/PhysRevC.89.044602

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  • Measurements of interaction cross sections for Na22-35 isotopes Reviewed

    S. Suzuki, M. Takechi, T. Ohtsubo, D. Nishimura, M. Fukuda, T. Kuboki, M. Nagashima, T. Suzuki, T. Yamaguchi, A. Ozawa, H. Ohishi, T. Moriguchi, T. Sumikama, H. Geissel, N. Aoi, Rui-Jiu Chen, De-Qing Fang, N. Fukuda, S. Fukuoka, H. Furuki, N. Inabe, Y. Ishibashi, T. Ito, T. Izumikawa, D. Kameda, T. Kubo, M. Lantz, C. S. Lee, Yu-Gang Ma, M. Mihara, S. Momota, D. Nagae, R. Nishikiori, T. Niwa, T. Ohnishi, K. Okumura, T. Ogura, H. Sakurai, K. Sato, Y. Shimbara, H. Suzuki, H. Takeda, S. Takeuchi, K. Tanaka, H. Uenishi, M. Winkler, Y. Yanagisawa

    INPC 2013 - INTERNATIONAL NUCLEAR PHYSICS CONFERENCE, VOL. 1   66   2014

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    Interaction cross sections (sigma(I)) for Na22-35 isotopes from the stability line to the vicinity of the neutron drip line have been measured at around 240 MeV/nucleon. The sigma(I) for Na33-35 were measured for the first time. Enhancement in cross sections is clearly observed from the systematics for stable nuclei, for isotopes with large mass numbers. From the known values of the nuclear-deformation parameters beta(2) of Na22-31, these enhancement can be mainly ascribed to the nuclear deformation. Large enhancement in heavier isotopes suggest that these nuclei are strongly deformed. The root-mean-square (RMS) nuclear matter radii were deduced from the sigma(I) by using Glauber-type calculation. Furthermore, a monotonic growth of the neutron-skin thickness has been deduced with increasing neutron number for Na isotopes.

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  • Neutron halo in B-14 studied via reaction cross sections Reviewed

    M. Fukuda, D. Nishimura, S. Suzuki, M. Tanaka, M. Takechi, K. Iwamoto, S. Wakabayashi, M. Yaguchi, J. Ohno, Y. Morita, Y. Kamisho, M. Mihara, K. Matsuta, M. Nagashima, T. Ohtsubo, T. Izumikawa, T. Ogura, K. Abe, N. Kikukawa, T. Sakai, D. Sera, T. Suzuki, T. Yamaguchi, K. Sato, H. Furuki, S. Miyazawa, N. Ichihashi, J. Kohno, S. Yamaki, A. Kitagawa, S. Sato, S. Fukuda

    INPC 2013 - INTERNATIONAL NUCLEAR PHYSICS CONFERENCE, VOL. 1   66   2014

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    Reaction cross sections (sigma(R)) for the neutron-rich nucleus B-14 on Be, C, and Al targets have been measured at several energies in the intermediate energy range of 45-120 MeV/nucleon. The present experimental sigma(R) show a significant enhancement relative to the systematics of stable nuclei. The nucleon density distribution was deduced through the fitting procedure with the modified Glauber calculation. The necessity of a long tail in the density distribution was found, which is consistent with the valence neutron in 2s(1/2) orbital with the small empirical one-neutron separation energy in B-14.

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  • First observation of an isomeric state in proton drip-line nucleus P-26 Reviewed

    D. Nishimura, M. Fukuda, T. Sakai, M. Tanaka, K. Abe, J. Chiba, S. Fukuda, H. Furuki, A. Homma, H. Hotaka, N. Ichihashi, N. Inaba, K. Iwamoto, T. Izumikawa, Y. Kamisho, K. Kanbe, N. Kikukawa, A. Kitagawa, J. Kouno, M. Nagashima, Y. Nakamura, I. Nishizuka, K. Matsuta, M. Mihara, S. Miyazawa, Y. Morita, J. Ono, T. Ohtsubo, K. Sato, S. Sato, D. Sera, S. Suzuki, S. Suzuki, T. Suzuki, M. Takechi, K. Tashiro, M. Wakabayashi, D. Watanabe, M. Yaguchi, T. Yamaguchi, S. Yamaki, S. Yasumoto, K. Yoshinaga, Y. Zhu

    INPC 2013 - INTERNATIONAL NUCLEAR PHYSICS CONFERENCE, VOL. 1   66   2014

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    An isomeric state in the proton drip-line nucleus P-26 has been observed by the gamma-ray spectroscopy. The gamma-ray energy and the half-life are 164.4 +/- 0.1 keV and 120 +/- 9 ns, respectively. For the isomeric transition of the mirror nucleus Na-26, the gamma-ray energy of 82.40 +/- 0.04 keV and the half-life of 4.35 +/- 0.16 mu s are also revised. Comparing the experimental reduced transition probabilities of Na-26 and P-26 with theoretical ones calculated by the shell model with the USDA interaction, the spin-parity (J(pi)) of the isomeric state in P-26 is most likely to be 1(+).

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  • Search for halo nucleus in Mg isotopes through the measurements of reaction cross sections towards the vicinity of neutron drip line Reviewed

    M. Takechi, S. Suzuki, D. Nishimura, M. Fukuda, T. Ohtsubo, M. Nagashima, T. Suzuki, T. Yamaguchi, A. Ozawa, T. Moriguchi, H. Ohishi, T. Sumikama, H. Geissel, N. Aoi, Rui-Jiu Chen, De-Qing Fang, N. Fukuda, S. Fukuoka, H. Furuki, N. Inabe, Y. Ishibashi, T. Itoh, T. Izumikawa, D. Kameda, T. Kubo, M. Lantz, Yu-Gang Ma, K. Matsuta, M. Mihara, S. Momota, R. Nishikiori, T. Niwa, T. Ohnishi, K. Okumura, M. Ohtake, T. Ogura, H. Sakurai, Y. Shimbara, H. Suzuki, H. Takeda, S. Takeuchi, K. Tanaka, H. Uenishi, M. Winkler, Y. Yanagisawa, S. Watanabe, K. Minomo, T. Sumi, S. Tagami, M. Kimura, T. Matsumoto, K. Ogata, Y. R. Shimizu, M. Yahiro

    INPC 2013 - INTERNATIONAL NUCLEAR PHYSICS CONFERENCE, VOL. 1   66   2014

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    Reaction cross sections (sigma R) for Mg24-38 on C targets at the energies of around 240 MeV/nucleon have been measured precisely at RIBF, RIKEN for the purpose of obtaining the crucial information on the changes of nuclear structure in unstable nuclei, especially around the so-called "island of inversion" region. In the island of inversion region, which includes neutron-rich Ne, Na, and Mg isotopes, the vanishing of the N = 20 magic number for neutrons have been discussed along with nuclear deformation. The present result suggest deformation features of Mg isotopes and shows a large cross section of weakly-bound nucleus Mg-37, which could be caused by a neutron halo formation.

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  • Charge-changing interactions probing point-proton radii of nuclei Reviewed

    S. Yamakil, J. Kouno, D. Nishimura, M. Nagashima, M. Takechi, K. Sato, K. Abe, Y. Abe, M. Fukuda, H. Furuki, I. Hachiuma, A. Homma, N. Ichihashi, C. Ichikawa, N. Inaba, T. Ito, K. Iwamoto, T. Izumikawa, Y. Kamisho, N. Kikuchi, S. Kinno, A. Kitagawa, T. Kojima, T. Kuboki, M. Mihara, S. Miyazawa, S. Momota, Y. Morita, D. Nagae, Y. Nakamura, K. Namihira, R. Nishikiori, I. Nishizuka, T. Niwa, M. Ogura, Y. Ohkuma, T. Ohtsubo, S. Okada, J. Ohno, A. Ozawa, Y. Saito, T. Sakai, S. Sato, D. Sera, F. Suzaki, S. Suzuki, S. Suzuki, T. Suzuki, M. Taguchi, H. Uenishi, M. Wakabayashi, D. Watanabe, M. Yaguchi, S. Yasumoto, T. Yamaguchi

    INPC 2013 - INTERNATIONAL NUCLEAR PHYSICS CONFERENCE, VOL. 1   66   2014

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    The question of whether charge-changing interactions can be used to probe point-proton radii of nuclei remains unanswered. Charge-changing cross sections, sigma(cc), were systematically investigated using stable and unstable nuclear beams of intermediate-energy. The ratios of the experimental sigma(cc) values to the calculated ones obtained from a phenomenological Glauber-type model analysis are found to be nearly constant in a broad range of Z/N for light neutron-rich nuclei. This enables the determination of density distributions, i.e., the radii of protons tightly bound in nuclei. To test the applicability of the present method to all nuclei in the nuclear chart, extensive measurements were performed for medium-mass nuclei ranging from Z = 18 to 32. The present study suggests the potential capability of a new experimental approach for exploring exotic nuclei.

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  • Systematic study of individual charge-changing cross sections of intermediate-energy secondary beams Reviewed

    S. Yamaki, T. Yamaguchi, J. Kouno, K. Sato, N. Ichihashi, T. Suzuki, K. Abe, Y. Abe, M. Fukuda, H. Furuki, N. Inaba, K. Iwamoto, T. Izumikawa, Y. Kamisho, N. Kikuchi, A. Kitagawa, M. Mihara, S. Miyazawa, S. Momota, Y. Morita, D. Nagae, M. Nagashima, Y. Nakamura, R. Nishikiori, D. Nishimura, I. Nishizuka, T. Ohtsubo, J. Ohno, A. Ozawa, T. Sakai, S. Sato, D. Sera, F. Suzaki, S. Suzuki, S. Suzuki, M. Wakabayashi, M. Yaguchi, S. Yasumoto

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B-BEAM INTERACTIONS WITH MATERIALS AND ATOMS   317   774 - 778   2013.12

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    Charge-changing interactions of stable and unstable medium-mass nuclides have been systematically investigated at intermediate energies. Secondary beams ranging from Ar to Ge isotopes produced by projectile fragmentation of Fe-56 and Ge-76 were irradiated onto a carbon target, and their total and partial charge-changing cross sections were precisely measured. A clear odd even effect found in the partial charge-changing cross sections monotonically varies as a function of the Z/N ratio among the isotopes, and grows toward the neutron-deficient side. The total charge-changing cross sections are sensitive to the Z number of nuclides, and tend to gradually increase toward the neutron-deficient side in some isotopes. (C) 2013 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nimb.2013.05.057

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  • Performance of high-resolution position-sensitive detectors developed for storage-ring decay experiments Reviewed

    T. Yamaguchi, F. Suzaki, T. Izumikawa, S. Miyazawa, K. Morimoto, T. Suzuki, F. Tokanai, H. Furuki, N. Ichihashi, C. Ichikawa, A. Kitagawa, T. Kuboki, S. Momota, D. Nagae, M. Nagashima, Y. Nakamura, R. Nishikiori, T. Niwa, T. Ohtsubo, A. Ozawa, K. Sato, S. Sato, S. Suzuki

    Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms   317   697 - 700   2013.12

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    DOI: 10.1016/j.nimb.2013.07.056

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  • Half-life measurements of highly charged radionuclides Reviewed

    D. R. Atanasov, D. Balabanski, L. Batist, K. Blaum, F. Bosch, D. Boutin, C. Brandau, C. Dimopoulou, H. G. Essel, T. Faestermann, H. Geissel, S. Hagmann, R. Hess, P-M Hillenbrand, P. Kienle, R. Knoebel, C. Kozhuharov, J. Kurcewicz, M. Lestinsky, S. A. Litvinov, Yu A. Litvinov, X. Ma, R. Maertin, M. Mazzocco, G. Muenzenberg, F. Nolden, T. Ohtsubo, Z. Patyk, M. S. Sanjari, C. Scheidenberger, D. Shubina, U. Spillmann, M. Steck, Th Stoehlker, B. Sun, T. Suzuki, S. Torilov, M. Trassinelli, S. Trotsenko, X. Tu, I. I. Tupitsyn, H. Weick, N. Winckler, M. Winkler, D. F. A. Winters, N. Winters, H. Xu, T. Yamaguchi, X. Yan, Y. Yuan, Y. Zhang

    PHYSICA SCRIPTA   T156   2013.9

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    In recent years several measurements of the orbital electron capture half-lives of few-electron ions have been carried out employing the storage ring ESR at GSI. Hydrogen-like and helium-like Pr-140 and Pm-142 as well as hydrogen-like I-122 were studied. Half-lives of the corresponding fully ionized nuclides provide the three-body beta(+) decay constants.

    DOI: 10.1088/0031-8949/2013/T156/014026

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  • Beta decay of highly charged ions Reviewed

    F. Bosch, D. R. Atanasov, C. Brandau, I. Dillmann, C. Dimopoulou, T. Faestermann, H. Geissel, S. Hagmann, P-M Hillenbrand, P. Kienle, R. Knoebel, C. Kozhuharov, J. Kurcewicz, M. Lestinsky, S. A. Litvinov, Yu A. Litvinov, X. Ma, F. Nolden, T. Ohtsubo, Z. Patyk, R. Reuschl, M. S. Sanjari, C. Scheidenberger, D. Shubina, U. Spillmann, M. Steck, Th Stoehlker, B. Sun, M. Trassinelli, S. Trotsenko, X. L. Tu, H. Weick, N. Winckler, M. Winkler, D. F. A. Winters, T. Yamaguchi, X. L. Yan

    PHYSICA SCRIPTA   T156   2013.9

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    A brief overview is presented in this paper on some experiments conducted at the Experimental Storage Ring (ESR) of GSI which addressed the beta decay of stored and cooled highly charged ions. Special emphasis is placed on the two-body beta decay of bare or few-electron ions: bound-state beta(-) decay (beta(b)) and its time-mirrored counterpart, orbital electron capture. The former decay mode was detected experimentally 20 years ago at the ESR. The latter could be investigated there for the first time in detail for the simplest quantum systems: hydrogen-and helium-like atoms. The main results of these experiments will be presented. Also their impact on stellar nucleosynthesis, in particular the s-process, is discussed.

    DOI: 10.1088/0031-8949/2013/T156/014025

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  • Density distributions of Li-11 deduced from reaction cross-section measurements Reviewed

    T. Moriguchi, A. Ozawa, S. Ishimoto, Y. Abe, M. Fukuda, I. Hachiuma, Y. Ishibashi, Y. Ito, T. Kuboki, M. Lantz, D. Nagae, K. Namihira, D. Nishimura, T. Ohtsubo, H. Ooishi, T. Suda, H. Suzuki, T. Suzuki, M. Takechi, K. Tanaka, T. Yamaguchi

    PHYSICAL REVIEW C   88 ( 2 )   2013.8

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    We measured the reaction cross sections of the two-neutron halo nucleus Li-11 with solid hydrogen and carbon targets at around 31 and 41 MeV/nucleon. The neutron density distribution of Li-11 was deduced for the first time by the Glauber model calculation based on the optical limit approximation. The uncertainty of the matter density of Li-11 was improved, compared with earlier measurements. The present root-mean-square radius of the proton distribution agrees with the previous one derived from an optical isotope shift measurement. The present root-mean-square radii reproduce theoretical calculations by the tensor optimized shell model by assuming core excitation. This consistency suggests the possibility that Li-9 in Li-11 is excited and the disappearance of the N = 8 shell gap of Li-11 is caused by correlations originating from the nucleon force, such as the tensor and the pairing.

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  • Magnetic Dipole Moment of the Doubly-Closed-Shell Plus One Proton Nucleus Sc-49 (vol 109, 032504, 2012) Reviewed

    T. Ohtsubo, N. J. Stone, J. R. Stone, I. S. Towner, C. R. Bingham, C. Gaulard, U. Koester, S. Muto, J. Nikolov, K. Nishimura, G. S. Simpson, G. Soti, M. Veskovic, W. B. Walters, F. Wauters

    PHYSICAL REVIEW LETTERS   110 ( 22 )   2013.5

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    DOI: 10.1103/PhysRevLett.110.229901

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  • Momentum dependence of spin polarization for beta emitting nuclei produced through charge exchange reaction at intermediate energy Reviewed

    S. Momota, M. Mihara, D. Nishimura, M. Fukuda, Y. Kamisho, M. Wakabayashi, K. Matsuta, S. Suzuki, M. Nagashima, Shengyun Zhu, Daqing Yuan, Yongnan Zheng, Zuo Yi, Ping Fan, T. Izumikawa, A. Kitagawa, S. Sato, M. Kanazawa, M. Torikoshi, T. Minamisono, Y. Nakamura, K. Tashiro, A. Honma, N. Yoshida, H. Shirai, T. Ohtsubo, T. Nagatomo, H. Uenishi, K. Iwamoto, M. Yaguchi, T. Ogura, T. Ito, K. Yamamura, Y. Ichikawa, Y. Nojiri, J. R. Alonso, T. J. M. Symons

    HYPERFINE INTERACTIONS   220 ( 1-3 )   53 - 58   2013.5

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    In order to investigate the polarization process in charge exchange reactions, we observed the momentum and angular distribution as well as the nuclear polarization of a proton-rich beta-emitting nucleus, P-28 (I (pi) = 3 (+) , T (1/2) = 270 msec), produced through the reaction Si-28+ Be-9 at E = 100 MeV/u, by selecting the momentum and the ejection angle. An analysis by using double Gaussian functions resolved the observed momentum distribution into two reaction components, nucleon knockout and pick-up abrasion reactions, as suggested in a previous study. The behavior of the observed angular distribution and nuclear polarization implies the influence of those two components. The momentum dependence of the observed nuclear polarization of P-28 could be consistently reproduced by a simple model, in which two reaction components are considered. The present study also shows that the charge exchange reaction at intermediate energy is a useful method to produce polarized beta-emitting nuclei, especially for proton-rich nuclei.

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  • Production of spin polarized N-12 through heavy ion reactions Reviewed

    M. Mihara, K. Matsuta, D. Nishimura, M. Fukuda, M. Yaguchi, K. Iwamoto, M. Wakabayashi, Y. Kamisho, J. Ohno, Y. Morita, T. Izumikawa, T. Ohtsubo, S. Suzuki, M. Nagashima, K. Abe, T. Sakai, S. Momota, A. Ozawa, D. Nagae, Y. Ishibashi, Y. Abe, T. Niwa, T. Nagatomo, T. Minamisono, M. K. Kubo, A. Kitagawa, M. Torikoshi, M. Kanazawa, S. Sato

    HYPERFINE INTERACTIONS   220 ( 1-3 )   83 - 88   2013.5

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    Production of spin polarized short-lived nucleus N-12 (I (pi) = 1 (+) , T (1/2) = 11 ms) using heavy ion reactions at intermediate energies has been performed. Typical polarization of about -25 % and +10 % through the projectile fragmentation Be(N-14, N-12)X and the charge exchange CH2(C-12, N-12)X processes, respectively, was obtained. The present study proved that the combination of a C-12 beam and a proton target provides a fairly good quality of polarized N-12 beam in terms of intensity and energy uniformity, and is promising for materials science use of N-12 as a nuclear probe.

    DOI: 10.1007/s10751-013-0869-7

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  • Direct observation of long-lived isomers in Bi212 Reviewed

    L. Chen, P. M. Walker, H. Geissel, Yu A. Litvinov, K. Beckert, P. Beller, F. Bosch, D. Boutin, L. Caceres, J. J. Carroll, D. M. Cullen, I. J. Cullen, B. Franzke, J. Gerl, M. Górska, G. A. Jones, A. Kishada, R. Knöbel, C. Kozhuharov, J. Kurcewicz, S. A. Litvinov, Z. Liu, S. Mandal, F. Montes, G. Münzenberg, F. Nolden, T. Ohtsubo, Z. Patyk, W. R. Plaß, Zs Podolyák, S. Rigby, N. Saito, T. Saito, C. Scheidenberger, E. C. Simpson, M. Shindo, M. Steck, B. Sun, S. J. Williams, H. Weick, M. Winkler, H. J. Wollersheim, T. Yamaguchi

    Physical Review Letters   110 ( 12 )   2013.3

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    Long-lived isomers in Bi212 have been studied following U238 projectile fragmentation at 670 MeV per nucleon. The fragmentation products were injected as highly charged ions into a storage ring, giving access to masses and half-lives. While the excitation energy of the first isomer of Bi212 was confirmed, the second isomer was observed at 1478(30) keV, in contrast to the previously accepted value of &gt
    1910 keV. It was also found to have an extended Lorentz-corrected in-ring half-life &gt
    30 min, compared to 7.0(3) min for the neutral atom. Both the energy and half-life differences can be understood as being due a substantial, though previously unrecognized, internal decay branch for neutral atoms. Earlier shell-model calculations are now found to give good agreement with the isomer excitation energy. Furthermore, these and new calculations predict the existence of states at slightly higher energy that could facilitate isomer deexcitation studies. © 2013 American Physical Society.

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  • NEW NEUTRON-RICH ISOMERS OBSERVED AMONG FISSION FRAGMENTS OF 345 MEV/U U-238 AND EVOLUTION OF NUCLEAR STRUCTURE Reviewed

    D. Kameda, T. Kubo, T. Ohnishi, K. Kusaka, A. Yoshida, K. Yoshida, M. Ohtake, N. Fukuda, H. Takeda, K. Tanaka, N. Inabe, Y. Yanagisawa, Y. Gono, H. Watanabe, H. Otsu, H. Baba, T. Ichihara, Y. Yamaguchi, M. Takechi, S. Nishimura, H. Ueno, A. Yoshimi, H. Sakurai, T. Motobayashi, T. Nakao, Y. Mizoi, M. Matsushita, K. Ieki, N. Kobayashi, K. Tanaka, Y. Kawada, N. Tanaka, S. Deguchi, Y. Satou, Y. Kondo, T. Nakamura, K. Yoshinaga, C. Ishii, H. Yoshii, Y. Miyashita, N. Uematsu, Y. Shiraki, T. Sumikama, J. Chiba, E. Ideguchi, A. Saito, T. Yamaguchi, I. Hachiuma, T. Suzuki, T. Moriguchi, A. Ozawa, T. Ohtsubo, M. A. Famiano, H. Geissel, A. S. Nettleton, O. B. Tarasov, D. Bazin, B. M. Sherrill, S. L. Manikonda, J. A. Nolen

    FISSION AND PROPERTIES OF NEUTRON-RICH NUCLEI, ICFN5   258 - +   2013

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  • Observation of new microsecond isomers among fission products from in-flight fission of 345 MeV/nucleon U-238 Reviewed

    D. Kameda, T. Kubo, T. Ohnishi, K. Kusaka, A. Yoshida, K. Yoshida, M. Ohtake, N. Fukuda, H. Takeda, K. Tanaka, N. Inabe, Y. Yanagisawa, Y. Gono, H. Watanabe, H. Otsu, H. Baba, T. Ichihara, Y. Yamaguchi, M. Takechi, S. Nishimura, H. Ueno, A. Yoshimi, H. Sakurai, T. Motobayashi, T. Nakao, Y. Mizoi, M. Matsushita, K. Ieki, N. Kobayashi, K. Tanaka, Y. Kawada, N. Tanaka, S. Deguchi, Y. Satou, Y. Kondo, T. Nakamura, K. Yoshinaga, C. Ishii, H. Yoshii, Y. Miyashita, N. Uematsu, Y. Shiraki, T. Sumikama, J. Chiba, E. Ideguchi, A. Saito, T. Yamaguchi, I. Hachiuma, T. Suzuki, T. Moriguchi, A. Ozawa, T. Ohtsubo, M. A. Famiano, H. Geissel, A. S. Nettleton, O. B. Tarasov, D. Bazin, B. M. Sherrill, S. L. Manikonda, J. A. Nolen

    PHYSICAL REVIEW C   86 ( 5 )   2012.11

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    A search for isomeric gamma decays among fission fragments from 345 MeV/nucleon U-238 has been performed at the RIKEN Nishina Center RI Beam Factory. Fission fragments were selected and identified using the superconducting in-flight separator BigRIPS and were implanted in an aluminum stopper. Delayed gamma rays were detected using three clover-type high-purity germanium detectors located at the focal plane within a time window of 20 mu s following the implantation. We identified a total of 54 microsecond isomers with half-lives of similar to 0.1-10 mu s, including the discovery of 18 new isomers in very neutron-rich nuclei: Ti-59(m), As-90(m), Se-92(m), Se-93(m), Br-94(m), Br-95(m), Br-96(m), Rb-97(m), Nb-108(m), Mo-109(m), Ru-117(m), Ru-119(m), Rh-120(m), Rh-122(m), Pd-121(m), Pd-124(m), Ag-124(m), and Ag-126(m), and obtained a wealth of spectroscopic information such as half-lives, gamma-ray energies, gamma-ray relative intensities, and gamma gamma coincidences over a wide range of neutron-rich exotic nuclei. Proposed level schemes are presented for Ti-59(m), Ga-82(m), Br-92(m), Br-94(m), Br-95(m), Rb-97(m), Rb-98(m), Nb-108(m), Zr-108(m), Mo-109(m), Ru-117(m), Ru-119(m), Rh-120(m), Rh-122(m), Pd-121(m), Ag-124(m), and Ag-125(m), based on the obtained spectroscopic information and the systematics in neighboring nuclei. The nature of the nuclear isomerism is discussed in relation to the evolution of nuclear structure.

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  • Magnetic Dipole Moment of the Doubly-Closed-Shell Plus One Proton Nucleus Sc-49 Reviewed

    T. Ohtsubo, N. J. Stone, J. R. Stone, I. S. Towner, C. R. Bingham, C. Gaulard, U. Koester, S. Muto, J. Nikolov, K. Nishimura, G. S. Simpson, G. Soti, M. Veskovic, W. B. Walters, F. Wauters

    PHYSICAL REVIEW LETTERS   109 ( 3 )   2012.7

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    The nucleus Sc-49, having a single f(7/2) proton outside doubly magic Ca-48 (Z = 20, N = 28), is one of the very few isotopes which makes possible testing of the fundamental theory of nuclear magnetism. The magnetic moment has been measured by online beta NMR of nuclei oriented at milli-Kelvin temperatures to be (+): 616(25) mu(N). The result is discussed in terms of a detailed theory of the structure of the magnetic moment operator, showing excellent agreement with calculated departure from the f(7/2) Schmidt limit extreme single-particle value. The measurement completes the sequence of moments of Sc isotopes with even numbers of f(7/2) neutrons: the first such isotopic chain between two major shells for which a full set of moment measurements exists. The result further completes the isotonic sequence of ground-state moments of nuclei with an odd number of f(7/2) protons coupled to a closed subshell of f(7/2) neutrons. Comparison with a recent shell-model calculation of the latter sequence is made.

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  • New results on mass measurements of stored neutron-rich nuclides in the element range from Pt to U with the FRS-ESR facility at 360-400 MeV/u Reviewed

    L. Chen, W. R. Plass, H. Geissel, R. Knoebel, C. Kozhuharov, Yu A. Litvinov, Z. Patyk, C. Scheidenberger, K. Siegien-Iwaniuk, B. Sun, H. Weick, K. Beckert, P. Beller, F. Bosch, D. Boutin, L. Caceres, J. J. Carroll, D. M. Cullen, I. J. Cullen, B. Franzke, J. Gerl, M. Gorska, G. A. Jones, A. Kishada, J. Kurcewicz, S. A. Litvinov, Z. Liu, S. Mandal, F. Montes, G. Muenzenberg, F. Nolden, T. Ohtsubo, Zs Podolyak, R. Propri, S. Rigby, N. Saito, T. Saito, M. Shindo, M. Steck, P. M. Walker, S. Williams, M. Winkler, H. -J. Wollersheim, T. Yamaguchi

    NUCLEAR PHYSICS A   882   71 - 89   2012.5

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    Masses of U-238 projectile fragments have been measured with time-resolved Schottky Mass Spectrometry (SMS) at the FRS-ESR facility at GSI. The exotic nuclei were created in the production target at the entrance of the fragment separator FRS, spatially separated in flight and injected into the storage-cooler ring ESR at about 70% light velocity. This means the ions were mainly bare or carried only a few electrons, e.g., the population of Li-like ions was below 1% for Pt fragments. Accurate new mass values of 33 neutron-rich, stored exotic nuclei in the element range from platinum to uranium have been obtained for the first time. In total more than 150 nuclides including references with well-known masses have been covered in this large-area SMS measurement. A novel data analysis has been applied which reduces the systematic errors by taking into account the velocity profile of the cooler electrons and the residual ion-optical dispersion in this part of the storage ring. The experiment, the data analysis, and the mass values are presented. The experimental data are compared with theoretical predictions demonstrating systematic deviations of up to 1500 keV from modern mass models. (C) 2012 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nuclphysa.2012.03.002

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  • Half-life measurements of stored fully ionized and hydrogen-like I-122 ions Reviewed

    D. R. Atanasov, N. Winckler, D. Balabanski, L. Batist, F. Bosch, D. Boutin, C. Brandau, C. Dimopoulou, H. G. Essel, T. Faestermann, H. Geissel, I. Hachiuma, S. Hess, T. Izumikawa, P. Kienle, R. Knoebel, C. Kozhuharov, J. Kurcewicz, N. Kuzminchuk, S. A. Litvinov, Yu. A. Litvinov, R. S. Mao, R. Maertin, M. Mazzocco, G. Muenzenberg, K. Namihira, F. Nolden, T. Ohtsubo, Z. Patyk, R. Reuschl, M. S. Sanjari, C. Scheidenberger, D. Shubina, U. Spillmann, M. Steck, Th. Stoehlker, B. Sun, T. Suzuki, M. Trassinelli, I. I. Tupitsyn, H. Weick, M. Winkler, D. F. A. Winters, T. Yamaguchi

    EUROPEAN PHYSICAL JOURNAL A   48 ( 2 )   2012.2

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    The half-lives of fully ionized and hydrogen-like (H-like) I-122 ions have been measured in a heavy-ion storage ring. The beta(+)-decay constants for both charge states and the electron capture (EC) decay constant of H-like ions have been determined. The EC-decay constant in H-like I-122 ions lambda(H-like)(EC) = 7.35(33) . 10(-4) s(-1) is, within the uncertainty, the same as the one in neutral atoms. This result is in agreement with the estimates of recent theoretical considerations on the EC-decay of few-electron ions that explicitly take into account the conservation of the total angular momentum of the nucleus plus lepton(s) system and its projections. No firm confirmation could be concluded from our results on the predicted effect that allowed Gamow-Teller transitions become forbidden if the initial and final total angular momenta are not equal.

    DOI: 10.1140/epja/i2012-12022-9

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  • Interaction cross sections for Ne isotopes towards the island of inversion and halo structures of Ne-29 and Ne-31 Reviewed

    M. Takechi, T. Ohtsubo, M. Fukuda, D. Nishimura, T. Kuboki, T. Suzuki, T. Yamaguchi, A. Ozawa, T. Moriguchi, H. Ooishi, D. Nagae, H. Suzuki, S. Suzuki, T. Izumikawa, T. Sumikama, M. Ishihara, H. Geissel, N. Aoi, Rui-Jiu Chen, De-Qing Fang, N. Fukuda, I. Hachiuma, N. Inabe, Y. Ishibashi, Y. Ito, D. Kameda, T. Kubo, K. Kusaka, M. Lantz, Yu-Gang Ma, K. Matsuta, M. Mihara, Y. Miyashita, S. Momota, K. Namihira, M. Nagashima, Y. Ohkuma, T. Ohnishi, M. Ohtake, K. Ogawa, H. Sakurai, Y. Shimbara, T. Suda, H. Takeda, S. Takeuchi, K. Tanaka, R. Watanabe, M. Winkler, Y. Yanagisawa, Y. Yasuda, K. Yoshinaga, A. Yoshida, K. Yoshida

    PHYSICS LETTERS B   707 ( 3-4 )   357 - 361   2012.2

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    Interaction cross sections (sigma(1)) for Me isotopes from the stability line to the vicinity of the neutron drip line have been measured at around 240 MeV/nucleon using BigRIPS at RIBF, RIKEN, The sigma(1) for Ne27-32 in every case exceed the systematic mass-number dependence of sigma(1) for stable nuclei, which can be explained by considering the nuclear deformation. In particular the sigma(1) for Ne-29 and Ne-31 are significantly greater than those of their neighboring nuclides. These enhancements of sigma(1) for Ne-29 and Ne-31 cannot be explained by a single-particle model calculation under the assumption that the valence neutron of Ne-29 (Ne-31) occupies the 0d(3/2) (0f(7/2)) orbital, as expected from the standard spherical shell ordering. The present data suggest an s dominant halo structure of Ne-29 and s- or p-orbital halo in Ne-31. (C) 2011 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.physletb.2011.12.028

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  • One- and two-neutron removal reactions from C-19,C-20 with a proton target Reviewed

    A. Ozawa, Y. Hashizume, Y. Aoki, K. Tanaka, T. Aiba, N. Aoi, H. Baba, B. A. Brown, M. Fukuda, K. Inafuku, N. Iwasa, T. Izumikawa, K. Kobayashi, M. Komuro, Y. Kondo, T. Kubo, M. Kurokawa, T. Matsuyama, S. Michimasa, T. Motobayashi, T. Nakabayashi, S. Nakajima, T. Nakamura, T. Ohtsubo, H. Sakurai, R. Shinoda, M. Shinohara, H. Suzuki, T. Suzuki, M. Takechi, E. Takeshita, S. Takeuchi, Y. Togano, K. Yamada, T. Yamaguchi, T. Yasuno, M. Yoshitake

    PHYSICAL REVIEW C   84 ( 6 )   2011.12

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    One-and two-neutron removal reactions from C-19 and C-20 have been studied using a liquid-hydrogen target at 40A MeV. A small cross section has been observed in the one-neutron removal reaction from C-20. The observed inclusive removal cross sections are compared with theoretical removal cross sections calculated by using shell model spectroscopic factors and Glauber-model single-particle cross sections. The observed momentum distributions are also compared with those calculated by using continuum-discretized coupled-channel methods. Good consistency between theory and experiment is shown in the one-neutron removal reaction from C-19. However, our theoretical calculation fails to reproduce the neutron removal reactions from C-20, which suggests that further improvements of the theoretical descriptions are necessary.

    DOI: 10.1103/PhysRevC.84.064315

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  • Nuclear reactions of C-19,C-20 on a liquid hydrogen target measured with the superconducting TOF spectrometer Reviewed

    T. Yamaguchi, K. Tanaka, T. Suzuki, A. Ozawa, T. Ohtsubo, T. Aiba, N. Aoi, H. Baba, M. Fukuda, Y. Hashizume, K. Inafuku, N. Iwasa, T. Izumikawa, K. Kobayashi, M. Komuro, Y. Kondo, T. Kubo, M. Kurokawa, T. Matsuyama, S. Michimasa, T. Motobayashi, T. Nakabayashi, S. Nakajima, T. Nakamura, H. Sakurai, R. Shinoda, M. Shinohara, H. Suzuki, M. Takechi, E. Takeshita, S. Takeuchi, Y. Togano, K. Yamada, T. Yasuno, M. Yoshitake

    NUCLEAR PHYSICS A   864 ( 1 )   1 - 37   2011.8

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    Reaction cross sections with various kinds of breakup channels for neutron-rich carbon isotopes C18-20 and for Be-9 impinging on a liquid hydrogen target were investigated at 40 MeV/nucleon. The nuclides of interest were produced via projectile fragmentation from a 63 MeV/nucleon Ar-40 beam and were separated in flight at the RIKEN projectile fragment separator (RIPS). The combination of the large-acceptance superconducting TOF spectrometer, TOMBEE (TOF Mass analyzer for exotic BEam Experiment), with a liquid hydrogen target, CRYPTA (CRYogenic ProTon and Alpha target system), enables simultaneous measurements of several reaction channels: the reaction cross sections (sigma(R)), individual elemental fragmentation cross sections (sigma(Delta Z)), charge-changing cross sections (sigma(cc)), neutron-removal cross sections (sigma(-xn)), and charge-pickup cross sections (sigma(Delta Z+i)) for C-19,C-20.sigma(Delta Z), sigma(-xn), and sigma(Delta Z)+1 for C-18; and sigma(R) for Be-9. The present sigma(R) of Be-9 on proton, sigma(R) = 397 +/- 23 mb, measured in the inverse kinematics, was consistent with the previous measurements using proton beams at different laboratories. The sigma(R) of C-19 and C-20 on proton were determined to be sigma(R) = 754 +/- 22 mb and sigma(R) = 791 +/- 34 mb, respectively. Taking into account the beam energy and target dependence of sigma(R), the present sigma(R) are found to be considerably enhanced compared with those measured at around I GeV/nucleon. The sigma Delta Z+1 appears to increase with the mass number of the projectiles, and it significantly contributes to sigma(R) in the present energy range. The finite-range optical-limit and few-body Glauber model analyses were performed for sigma(R) to study the nuclear matter density distributions and to derive the relative strength of the s-wave components of the valence neutrons in C-19 and C-20. A neutron halo structure of C-19 is confirmed with an s-wave dominance of the valence neutron when the effect of the charge-pickup reaction is taken into account. The large sigma(-n) of C-19 and sigma(-2n) of C-20 also support the decoupled structures of C-18 + n and C-18 + 2n, respectively. The sigma(cc) of C-19 and C-20 agree with each other within their experimental uncertainties, which might indicate a similar proton density distribution in C-19 and C-20. The sigma(Delta Z) decreases monotonically without the even odd effect as the number of removed protons increases. (C) 2011 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nuclphysa.2011.05.095

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  • MEASUREMENT OF INTERACTION CROSS-SECTIONS FOR NEUTRON-RICH Na ISOTOPES Reviewed

    T. Kuboki, T. Ohtsubo, M. Takechi, I. Hachiuma, K. Namihira, T. Suzuki, T. Yamaguchi, Y. Ohkuma, Y. Shimbara, S. Suzuki, R. Watanabe, M. Fukuda, M. Mihara, D. Nishimura, Y. Ishibashi, Y. Ito, T. Moriguchi, D. Nagae, H. Ooishi, K. Ogawa, A. Ozawa, Y. Yasuda, H. Suzuki, T. Sumikama, K. Yoshinaga, H. Geissel, M. Winkler, T. Izumikawa, S. Momota, N. Aoi, N. Fukuda, N. Inabe, D. Kameda, K. Kusaka, T. Kubo, M. Lantz, T. Ohnishi, M. Ohtake, T. Suda, H. Takeda, K. Tanaka, Y. Yanagisawa, A. Yoshida, K. Yoshida

    ACTA PHYSICA POLONICA B   42 ( 3-4 )   765 - 768   2011.3

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    The interaction cross-sections (sigma(I)) of neutron-rich Na isotopes, (23-35)Na, on C target have been measured at 250A MeV using the RI beam factory (RIBF) at RIKEN. Mass dependence of sigma(I) for (27-35)Na suggests monotonic growth of the skin thickness. The root-mean-square nuclear matter radii ((r) over tilde (m)) of (23-35)Na were deduced from observed sigma(I) via a Glauber-type calculation. These (r) over tilde (m) are in a good agreement with the theoretical prediction by relativistic mean field model (RMF). (r) over tilde (m) of (33-35)Na were determined for the first time.

    DOI: 10.5506/APhysPolB.42.765

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  • Density distribution of Ne-17 and possible shell-structure change in the proton-rich sd-shell nuclei Reviewed

    K. Tanaka, M. Fukuda, M. Mihara, M. Takechi, D. Nishimura, T. Chinda, T. Sumikama, S. Kudo, K. Matsuta, T. Minamisono, T. Suzuki, T. Ohtsubo, T. Izumikawa, S. Momota, T. Yamaguchi, T. Onishi, A. Ozawa, I. Tanihata, T. Zheng

    PHYSICAL REVIEW C   82 ( 4 )   2010.10

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    Reaction cross sections (sigma(R)) for the proton drip-line nucleus Ne-17 have been measured on Be-9, C-12, and Al-27 targets at 64 and 42 MeV/nucleon by the transmission method. From the energy dependence of the sigma(R) including the high energy data, the density distribution of Ne-17 was deduced through a modified Glauber-type calculation. It is indicated that Ne-17 has a long tail in the density, consistent with a (2s(1/2))(2)-dominant configuration of two valence protons.

    DOI: 10.1103/PhysRevC.82.044309

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  • Discovery and investigation of heavy neutron-rich isotopes with time-resolved Schottky spectrometry in the element range from thallium to actinium Reviewed

    L. Chen, W. R. Plass, H. Geissel, R. Knoebel, C. Kozhuharov, Yu. A. Litvinov, Z. Patyk, C. Scheidenberger, K. Siegien-Iwaniuk, B. Sun, H. Weick, K. Beckert, P. Beller, F. Bosch, D. Boutin, L. Caceres, J. J. Carroll, D. M. Cullen, I. J. Cullen, B. Franzke, J. Gerl, M. Gorska, G. A. Jones, A. Kishada, J. Kurcewicz, S. A. Litvinov, Z. Liu, S. Mandal, F. Montes, G. Muenzenberg, F. Nolden, T. Ohtsubo, Zs. Podolyak, R. Propri, S. Rigby, N. Saito, T. Saito, M. Shindo, M. Steck, P. Ugorowski, P. M. Walker, S. Williams, M. Winkler, H. -J. Wollersheim, T. Yamaguchi

    PHYSICS LETTERS B   691 ( 5 )   234 - 237   2010.8

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    (238)U projectile fragments have been created at the entrance of the fragment separator FRS, spatially separated in flight within 0.45 mu s and injected into the storage-cooler ring ESR at 7.9 Tm corresponding to about 70% light velocity. Accurate new mass values and lifetime information of the stored exotic nuclei in the element range from platinum to uranium have been obtained with single-particle Schottky spectrometry. In this experiment the new isotopes of (236)AC, (224)At, (221)Po, (222)po, and (213)Tl were discovered. The isotopes were unambiguously identified and their masses measured. In addition, the time-correlated data have provided information on the lifetime of the new nuclides. The discovery of isotopes along with accurate mass measurement has been achieved for the first time at the FRS-ESR facility. The results will contribute to the knowledge of the decay products from the r-process nuclei and enable a crucial test of the predictive power of modern nuclear mass and half-life models. (C) 2010 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.physletb.2010.05.078

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  • MEASUREMENTS OF INTERACTION CROSS SECTIONS TOWARDS NEUTRON-RICH Ne ISOTOPES AT RIBF Reviewed

    M. Takechi, T. Ohtsubo, T. Kuboki, M. Fukuda, D. Nishimura, T. Suzuki, T. Yamaguchi, A. Ozawa, T. Moriguchi, T. Sumikama, H. Geissel, N. Aoi, N. Fukuda, I. Hachiuma, N. Inabe, Y. Ishibashi, Y. Itoh, D. Kameda, T. Kubo, K. Kusaka, M. Lantz, M. Mihara, Y. Miyashita, S. Momota, K. Namihira, H. Ohishi, Y. Ohkuma, T. Ohnishi, M. Ohtake, K. Ogawa, Y. Shimbara, T. Suda, S. Suzuki, H. Takeda, K. Tanaka, R. Watanabe, M. Winkler, Y. Yanagisawa, Y. Yasuda, K. Yoshinaga, A. Yoshida, K. Yoshida

    MODERN PHYSICS LETTERS A   25 ( 21-23 )   1878 - 1881   2010.7

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    Interaction cross sections (sigma(I)) for Ne isotopes from the stability line to the vicinity of neutron-drip line have been measured using the RIBF facility at RIKEN. Measurements have been performed for (20-32)Ne on C target at energies around 240 MeV/nucleon. A large enhancement of sigma(I) beyond the systematics of stable nuclei have been observed for neutron-rich Ne isotopes. The possible halo structures with lower orbital angular momentum for (29,31)Ne are discussed by the preliminary analysis.

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  • Identification of 45 New Neutron-Rich Isotopes Produced by In-Flight Fission of a U-238 Beam at 345 MeV/nucleon Reviewed

    Tetsuya Ohnishi, Toshiyuki Kubo, Kensuke Kusaka, Atsushi Yoshida, Koichi Yoshida, Masao Ohtake, Naoki Fukuda, Hiroyuki Takeda, Daisuke Kameda, Kanenobu Tanaka, Naohito Inabe, Yoshiyuki Yanagisawa, Yasuyuki Gono, Hiroshi Watanabe, Hideaki Otsu, Hidetada Baba, Takashi Ichihara, Yoshitaka Yamaguchi, Maya Takechi, Shunji Nishimura, Hideki Ueno, Akihiro Yoshimi, Hiroyoshi Sakurai, Tohru Motobayashi, Taro Nakao, Yutaka Mizoi, Masafumi Matsushita, Kazuo Ieki, Nobuyuki Kobayashi, Kana Tanaka, Yosuke Kawada, Naoki Tanaka, Shigeki Deguchi, Yoshiteru Satou, Yosuke Kondo, Takashi Nakamura, Kenta Yoshinaga, Chihiro Ishii, Hideakira Yoshii, Yuki Miyashita, Nobuya Uematsu, Yasutsugu Shiraki, Toshiyuki Sumikama, Junsei Chiba, Eiji Ideguchi, Akito Saito, Takayuki Yamaguchi, Isao Hachiuma, Takeshi Suzuki, Tetsuaki Moriguchi, Akira Ozawa, Takashi Ohtsubo, Michael A. Famiano, Hans Geissel, Anthony S. Nettleton, Oleg B. Tarasov, Daniel P. Bazin, Bradley M. Sherrill, Shashikant L. Manikonda, Jerry A. Nolen

    JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN   79 ( 7 )   2010.7

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    A search for new isotopes using in-flight fission of a 345 MeV/nucleon U-238 beam has been carried out at the RI Beam Factory at the RIKEN Nishina Center. Fission fragments were analyzed and identified by using the superconducting in-flight separator BigRIPS. We observed 45 new neutron-rich isotopes: Mn-71, Fe-73,Fe-74, Co-76, Ni-79, Cu-81,Cu-82, Zn-84,Zn-85, Ga-87, Ge-90, Se-95, Br-98, Kr-101, Rb-103, Sr-106,Sr-107, Y-108,Y-109, Zr-111,Zr-112, Nb-114,Nb-115, Mo-115,Mo-116,Mo-117, Tc-119,Tc-120, (121,122,123),Ru-124, Rh-123,Rh-124,Rh-125,Rh-126, Pd-127,Pd-128, Cd-133, Sn-138, Sb-140, Te-143, I-145, Xe-148, and Ba-152.

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  • Energy-dependent charge-changing cross sections and proton distribution of Si-28 Reviewed

    T. Yamaguchi, M. Fukuda, S. Fukuda, G. W. Fan, I. Hachiuma, M. Kanazawa, A. Kitagawa, T. Kuboki, M. Lantz, M. Mihara, M. Nagashima, K. Namihira, D. Nishimura, Y. Okuma, T. Ohtsubo, S. Sato, T. Suzuki, M. Takechi, W. Xu

    PHYSICAL REVIEW C   82 ( 1 )   2010.7

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    The charge-changing cross sections (sigma(cc)) of Si-28 on a carbon target were measured with high precision at intermediate energies from 100 to 600 MeV/nucleon. The measured scc decreases rapidly from low energies up to 200 MeV/nucleon, whereas at higher energies it appears almost constant. The energy dependence of scc is compared with a Glauber-type model calculation where only the proton distribution of Si-28 is taken into account. A phenomenological correction factor deduced from the present data satisfactorily reproduces the experimental scc for other stable nuclei, whose charge distributions were determined by electron scattering and muon capture experiments.

    DOI: 10.1103/PhysRevC.82.014609

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  • EXOTIC NUCLEAR STRUCTURES OF LIGHT UNSTABLE NUCLEI VIA REACTION CROSS SECTION MEASUREMENT Reviewed

    D. Nishimura, M. Fukuda, M. Takechi, M. Mihara, J. Komurasaki, R. Matsumiya, K. Matsuta, I. Hachimuma, T. Kuboki, M. Miura, S. Nakajima, K. Namihira, K. Saito, T. Suzuki, T. Yamaguchi, M. Yoshitake, M. Nagashima, Y. Ohkuma, T. Ohtsubo, Y. Shinbara, R. Watanabe, T. Izumikawa, M. Lantz, K. Tanaka, T. Suda, T. Moriguchi, A. Ozawa, D. Ishikawa, Y. Yasuda, S. Momota, S. Fukuda, M. Kanazawa, A. Kitagawa, S. Sato

    MODERN PHYSICS LETTERS A   25 ( 21-23 )   2014 - 2015   2010.7

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    Reaction cross sections for (11)Be and (8)B on proton targets at 40A - 120A MeV have been measured by the transmission method. With these data, we can discuss the proton-and neutron-density distributions at the nuclear surface independently in principle using the Glauber theory. Our experimental results support that the constituent of halo in (11)Be is neutron dominantly and that of (8)B is proton dominantly.

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  • Polarization creation in proton-rich P-28 via charge exchange reactions and measurement of its electric quadrupole moment Reviewed

    K. Matsuta, M. Mihara, D. M. Zhou, Y. N. Zheng, D. Nishimura, T. Nagatomo, D. Q. Yuan, S. Momota, T. Izumikawa, Y. Zuo, P. Fan, S. Y. Zhu, T. Ohtsubo, M. Fukuda, Y. Namiki, M. Nagashima, T. Minamisono, D. Kameda, T. Sumikama, A. Kitagawa, M. Kanazawa, M. Torikoshi, S. Sato, R. Matsumiya, J. Komurasaki, D. Ishikawa, H. Hirano, S. Takahashi, T. Kubo, R. Yamada, Y. Shimbara, Y. Nojiri, T. Suzuki, X. Z. Zhang, J. R. Alonso, G. F. Krebs, T. J. M. Symons

    HYPERFINE INTERACTIONS   198 ( 1-3 )   147 - 151   2010.6

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    The degrees of polarization of proton rich nucleus P-28 produced in charge exchange reactions Si-28 + Be-9 -> P-28 + X, and Si-28 + H-1 -> P-28 + X have been observed at 100 A MeV. Utilizing thus obtained polarized nuclei, the magnetic moment of P-28 was remeasured, and vertical bar mu(P-28)vertical bar = 0.3115 (34) mu(N) was obtained. beta-nuclear quadrupole resonance (beta-NQR) of P-28 implanted in alpha-Al2O3 have been observed for the first time, in order to measure the electric quadrupole moment of this nucleus.

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  • NMR-ON study of (PtNi)-Pt-197 Reviewed

    T. Ohtsubo, S. Ohya, Y. Masamori, T. Izumikawa, S. Muto, K. Nishimura

    HYPERFINE INTERACTIONS   198 ( 1-3 )   143 - 146   2010.6

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    Nuclear magnetic resonance measurement has been performed for Pt-197 oriented at 7 mK in a Ni host. The magnetic hyperfine splitting frequency at external magnetic fields of 0.2, 0.4 and 0.6 T were determined to be 229.4(1), 228.2(2) and 226.9(3) MHz, respectively. By using published values of the magnetic resonance frequency of (PtNi)-Pt-197 and magnetic moments determined by atomic beam methods, the hyperfine anomaly between the two isotopes is deduced to be (191)Delta(197) = +13(5)%. Which is extremely large compared to the theoretical value of +0.2%. Based on the same reasoning, the hyperfine anomaly with Pt-195, an isotope with the same spin and parity, is found to be (195)Delta(197) = +15(5)%. We conclude therefore that the published magnetic moment of Pt-197 is more likely in error. If we assume the hyperfine anomaly (195)Delta(197) = 0, a magnetic moment mu(Pt-191) = 0.45(1) mu(N) is obtained.

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  • Direct measurement of the 4.6 MeV isomer in stored bare Sb-133 ions Reviewed

    B. Sun, R. Knoebel, H. Geissel, Yu. A. Litvinov, P. M. Walker, K. Blaum, F. Bosch, D. Boutin, C. Brandau, L. Chen, I. J. Cullen, A. Dolinskii, B. Fabian, M. Hausmann, C. Kozhuharov, J. Kurcewicz, S. A. Litvinov, Z. Liu, M. Mazzocco, J. Meng, F. Montes, G. Muenzenberg, A. Musumarra, S. Nakajima, C. Nociforo, F. Nolden, T. Ohtsubo, A. Ozawa, Z. Patyk, W. R. Plass, C. Scheidenberger, M. Steck, T. Suzuki, H. Weick, N. Winckler, M. Winkler, T. Yamaguchi

    PHYSICS LETTERS B   688 ( 4-5 )   294 - 297   2010.5

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    The core-excited isomer in fully-ionized Sb-133 has been directly studied for the first time by applying the novel technique of isochronous mass spectrometry at GSI. The neutron-rich nuclides in high charge states were produced by projectile fission of 411 MeV A U-238 ions, separated in flight by the fragment separator (FRS) and stored in the isochronous storage ring (ESR). The measured excitation energy is 4.56(10) MeV. The neutral-atom half-life is known to be 17 mu s. This is the shortest-lived isomer measured directly with mass spectrometry techniques. The extended in-flight half-life of the bare ions in the ESR, which is due to the exclusion of the strong internal conversion, demonstrates that there should be another nuclear level above that identified from isomer-decay spectroscopy, in support of shell-model calculations. This measurement opens up a new half-life domain for storage-ring measurements. (c) 2010 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.physletb.2010.04.020

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  • Magnetic hyperfine interaction of Fe-59 in nickel Reviewed

    Suguru Muto, Susumu Ohya, Takashi Ohtsubo, Takuji Izumikawa, Katsuhiko Nishimura

    HYPERFINE INTERACTIONS   197 ( 1-3 )   117 - 121   2010.4

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    Nuclear magnetic resonance on oriented nuclei (NMR-ON) on Fe-59 isotope in Ni was performed. The magnetic hyperfine splitting frequency of was determined to be nu(B-0 = 0) = 48.32 (2) MHz. Using the known magnetic moment the magnetic hyperfine field was deduced as B-HF = -28.32 (5) T. The effective nuclear spin-lattice relaxation time was also measured. The measured value is compared with experimental values of 3d-impurity in nickel host.

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  • Beta-NMR measurement of Cu-58 in Si Reviewed

    M. Mihara, T. Izumikawa, H. Ueno, K. Matsuta, D. Nishimura, T. Nagatomo, T. Moriguchi, Y. Ito, D. Nagae, M. Fukuda, A. Yoshimi, K. Yamada, M. Takechi, Y. Ichikawa, S. Momota, Y. Hirayama, T. Ohtsubo, S. Suzuki, T. Kubo, Y. Namiki, A. Ozawa, Y. Ishibashi, H. Oishi, K. Suzuki, I. Hachiuma, K. Namihira, D. Horikawa, T. Minamisono, T. Yamaguchi, T. Kuboki, T. Suzuki, K. Satoh, Y. Kobayashi, K. Asahi, K. Matsukawa, K. Shirai

    HYPERFINE INTERACTIONS   197 ( 1-3 )   143 - 147   2010.4

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    The beta-NMR study of short-lived nucleus Cu-58 (I-pi = 1(+), T-1/2 = 3.2 s) in Si has been performed. Spin polarization of Cu-58 induced by the charge exchange reaction of Ni-58 was observed in Si at 15 K. The Cu-58 magnetic moment |mu[Cu-58]vertical bar = (0.46 +/- 0.03)mu(N) deduced from the beta-NMR spectrum is consistent with the previous results on the laser spectroscopy. The present result shows that the Cu-58 nucleus is promising as a new nuclear probe for the microscopic study of Cu impurities in Si.

    DOI: 10.1007/s10751-010-0249-5

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  • Nuclear structure and fundamental symmetry studied through nuclear moments Reviewed

    K. Matsuta, M. Mihara, M. Fukuda, D. Nishimura, R. Matsumiya, T. Nagatomo, T. Ohtsubo, T. Izumikawa, S. Momota, D. M. Zhou, D. Q. Yuan, Y. N. Zheng, Y. Zuo, P. Fan, S. Y. Zhu, A. Kitagawa, M. Kanazawa, M. Torikoshi, S. Sato, K. Minamisono, T. Sumikama, M. Ogura, M. Tanigaki, A. Ozawa, T. Yamaguchi, T. Suzuki, K. Tanaka, Maya Takechi, T. Minamisono, Y. Nojiri, P. Levy, T. J. M. Symons, J. R. Alonso, G. F. Krebs

    NUCLEAR PHYSICS A   834 ( 1-4 )   424C - 427C   2010.3

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    We report recent situation of anomaly in spin expectation value found in C-9-Li-9 mirror pair, recent analysis of the nuclear spin in terms of orbital or intrinsic and proton or neutron, and a result from the study of the G-parity conservation law through beta-ray angular correlation in terms of its nuclear orientation.

    DOI: 10.1016/j.nuclphysa.2010.01.055

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  • Distinction between Proton-Neutron Density Distribution of Halo Nuclei at the Nuclear Surface via Reaction Cross Sections Reviewed

    D. Nishimura, M. Fukuda, M. Takechi, M. Mihara, D. Ishikawa, J. Komurasaki, K. Matsuta, R. Matsumiya, T. Kuboki, M. Yoshitake, T. Suzuki, T. Yamaguchi, S. Nakajima, K. Saito, M. Miura, I. Hachiuma, K. Namihira, T. Ohtsubo, Y. Shimbara, R. Watanabe, Y. Ohkuma, T. Izumikawa, K. Tanaka, T. Suda, A. Ozawa, Y. Yasuda, T. Moriguchi, S. Momota, S. Fukuda, S. Sato, M. Kanazawa, A. Kitagawa

    NUCLEAR PHYSICS A   834 ( 1-4 )   470C - 472C   2010.3

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    Reaction cross sections (sigma(R)) for Be-11 and B-8 on proton targets at 50A similar to 120A MeV have been measured to distinguish between the proton- and neutron- density distributions at the nuclear surface. The sigma(R) is connected with the nucleon density distributions by the Glauber theory. Since the nucleon-nucleon total cross sections in that energy region have a large isospin dependence, the sigma(R) on proton targets should have a large difference between the proton and neutron in the halo structure. The experimental sigma(R) on proton targets are in good agreement with the calculated ones assuming that the tail dominantly consists of a neutron for Be-11 and a proton for B-8.

    DOI: 10.1016/j.nuclphysa.2010.01.067

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  • Nuclear spin-lattice relaxation of light impurities in platinum studied by using polarized unstable nuclear beams Reviewed

    M. Mihara, K. Matsuta, D. Nishimura, H. Hirano, J. Komurasaki, S. Takahashi, T. Nagatomo, R. Matsumiya, M. Ogura, H. Akai, S. Momota, T. Ohtsubo, Y. Izumikawa, Dongmei Zhou, Yongnan Zheng, Daqing Yuan, Ping Fan, Yi Zuo, Shengyun Zhu, A. Kitagawa, M. Kanazawa, M. Torikoshi, S. Sato, M. Fukuda, D. Ishikawa, T. Minamisono, R. Watanabe, T. Kubo, Y. Nojiri, T. Sumikama, J. R. Alonso, G. F. Crebs, T. J. M. Symons

    NUCLEAR PHYSICS A   834 ( 1-4 )   777C - 779C   2010.3

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    The spin lattice-relaxation rates of short-lived unstable nuclei Al-25 and (28)p if, Pt has been measured by means of the beta-NMR technique, in order to study the electronic structure of dilute impurities in Pt. From the obtained spin-lattice relaxation rates, Knight shifts K-c were estimated to be K-c[Al in Pt] = (0.45 +/- 0.09)x10(-3) and K-c[P in Pt] = (4 +/- 2 4) x 10(-3) using the Korringa relation. These values were evaluated by comparing to the first principle Calculations.

    DOI: 10.1016/j.nuclphysa.2010.01.144

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  • Measurements of nuclear radii for neutron-rich Ne isotopes Ne28-32 Reviewed

    M. Takechi, T. Ohtsubo, T. Kuboki, M. Fukuda, D. Nishimura, T. Suzuki, T. Yamaguchi, A. Ozawa, T. Moriguchi, T. Sumikama, H. Geissel, N. Aoi, N. Fukuda, I. Hachiuma, N. Inabe, Y. Ishibashi, Y. Itoh, D. Kameda, K. Kusaka, M. Lantz, M. Mihara, Y. Miyashita, S. Momota, K. Namihira, H. Ohishi, Y. Ohkuma, T. Ohnishi, M. Ohtake, K. Ogawa, Y. Shimbara, T. Suda, S. Suzuki, H. Takeda, K. Tanaka, R. Watanabe, M. Winkler, Y. Yanagisawa, Y. Yasuda, K. Yoshinaga, A. Yoshida, K. Yoshida, T. Kubo

    NUCLEAR PHYSICS A   834 ( 1-4 )   412C - 415C   2010.3

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    Interaction cross sections (sigma(I)) for neutron-rich Ne isotopes, Ne28-32 on C target have been measured at 240A MeV using the RIBF at RIKEN. A large enhancement of sigma(I) beyond the systematics of stable nuclei have been observed for neutron-rich Ne isotopes, particularly for Ne-31. The possible halo structure for Ne-29,Ne-31 which would be caused by the lowering of the pf-shell and nuclear deformation of Ne isotopes are discussed by the preliminary analysis.

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  • Electromagnetic moments of F-22 Reviewed

    M. Mihara, K. Matsuta, J. Komurasaki, H. Hirano, D. Nishimura, S. Momota, T. Ohtsubo, T. Izumikawa, Y. Shimbara, T. Kubo, D. Kameda, Dongmei Zhou, Yongnan Zheng, Daqing Yuan, Shengyun Zhu, A. Kitagawa, M. Kanazawa, M. Torikoshi, S. Sato, T. Nagatomo, R. Matsumiya, D. Ishikawa, M. Fukuda, T. Minamisono, Y. Nojiri, J. R. Alonso, G. F. Crebs, T. J. M. Symons

    NUCLEAR PHYSICS A   834 ( 1-4 )   75C - 77C   2010.3

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    The magnetic dipole (mu) and electric quadrupole (Q) moments of short-lived nucleus F-22 (I-pi = 4(+), T-1/2 = 4.2 s) have been measured for the first time by means of the beta-NMR technique. A spin polarized F-22 beam was produced through the charge exchange reaction of Ne-22 and was implanted into single crysltals of NaF and MgF2 for mu and Q measurements, respectively. As a result,vertical bar mu(F-22)vertical bar = (2.69443 +/- 0.00039)mu(N) and vertical bar Q(F-22)vertical bar = (3 +/- 2) mb was obtained. These values are well reproduced by the shell model calculations.

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  • Directional correlation of nuclear-collision probability for aligned beams of deformed nucleus Reviewed

    M. Fukuda, D. Nishimura, M. Takechi, M. Mihara, K. Matsuta, R. Matsumiya, T. Kuboki, K. Namihira, I. Hachiuma, T. Yamaguchi, T. Suzuki, Y. Okuma, M. Nagashima, T. Ohtsubo, Y. Shimbara, T. Izumikawa, K. Tanaka, T. Suda, S. Momota, T. Minamisono, W. Xu, G. W. Fan, S. Fukuda, S. Sato, M. Kanazawa, A. Kitagawa

    NUCLEAR PHYSICS A   834 ( 1-4 )   461C - 463C   2010.3

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    Interaction cross sections have been measured for spin-aligned nuclear beams of deformed nucleus. The spin-aligned nuclear beams were created by selecting the momentum of fragments produced in the projectile fragmentation of intermediate energy heavy-ion beams. The directional correlation of nuclear reaction probability for heavy-ion beams of deformed nucleus has been directly observed for the first time.

    DOI: 10.1016/j.nuclphysa.2010.01.064

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  • Observation of a Large Reaction Cross Section in the Drip-Line Nucleus C-22 Reviewed

    K. Tanaka, T. Yamaguchi, T. Suzuki, T. Ohtsubo, M. Fukuda, D. Nishimura, M. Takechi, K. Ogata, A. Ozawa, T. Izumikawa, T. Aiba, N. Aoi, H. Baba, Y. Hashizume, K. Inafuku, N. Iwasa, K. Kobayashi, M. Komuro, Y. Kondo, T. Kubo, M. Kurokawa, T. Matsuyama, S. Michimasa, T. Motobayashi, T. Nakabayashi, S. Nakajima, T. Nakamura, H. Sakurai, R. Shinoda, M. Shinohara, H. Suzuki, E. Takeshita, S. Takeuchi, Y. Togano, K. Yamada, T. Yasuno, M. Yoshitake

    PHYSICAL REVIEW LETTERS   104 ( 6 )   2010.2

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    Reaction cross sections (sigma(R)) for C-19, C-20 and the drip-line nucleus C-22 on a liquid hydrogen target have been measured at around 40A MeV by a transmission method. A large enhancement of sigma(R) for C-22 compared to those for neighboring C isotopes was observed. Using a finite-range Glauber calculation under an optical-limit approximation the rms matter radius of C-22 was deduced to be 5.4 +/- 0.9 fm. It does not follow the systematic behavior of radii in carbon isotopes with N <= 14, suggesting a neutron halo. It was found by an analysis based on a few-body Glauber calculation that the two-valence neutrons in C-22 preferentially occupy the 1s(1/2) orbital.

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  • Reaction cross section studies at NIRS and RIBF Reviewed

    M. Fukuda, M. Takechi, D. Nishimura, M. Mihara, R. Matsumiya, K. Matsuta, T. Minamisono, T. Ohtsubo, Y. Ohkuma, Y. Shimbara, S. Suzuki, R. Watanabe, T. Izumikawa, S. Momota, T. Suzuki, T. Yamaguchi, T. Kuboki, I. Hachiuma, K. Namihira, S. Nakajima, K. Kobayashi, T. Sumikama, Y. Miyashita, K. Yoshinaga, K. Tanaka, N. Aoi, N. Fukuda, N. Inabe, D. Kameda, T. Kubo, K. Kusaka, M. Lantz, T. Ohnishi, M. Ohtake, T. Suda, H. Takeda, Y. Yanagisawa, A. Yoshida, K. Yoshida, A. Ozawa, T. Moriguchi, H. Ohishi, Y. Itoh, Y. Ishibashi, K. Ogawa, Y. Yasuda, H. Geissel, M. Winkler, S. Sato, M. Kanazawa, A. Kitagawa

    TOURS SYMPOSIUM ON NUCLEAR PHYSICS AND ASTROPHYSICS - VII   1238   270 - +   2010

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    Reaction cross sections for stable nuclei at intermediate energies have been measured precisely and systematically. The data have been found to be reproduced nicely by the optical-limit approximation of Glauber theory modified to include the nucleon multiple scattering effect and the Fermi-motion effect. Applying this prescription, the nucleon density distribution of Ne-17 has been studied. The surface structure of B-8 and Be-11 has been also studied using this prescription and hydrogen targets. Using the RIBF that has just started application to studies of exotic nuclei, neutron-rich Ne isotopes around the Island of Inversion have been investigated through measurements of their interaction cross sections.

    DOI: 10.1063/1.3455949

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  • Decay curve study in a standard electron capture decay Reviewed

    D. Nishimura, M. Fukuda, T. Izumikawa, K. Kisamori, Y. Kuwada, K. Makisaka, R. Matsumiya, K. Matsuta, M. Mihara, T. Ohtsubo, T. Suzuki, A. Takagi, T. Yamaguchi, R. Yokoyama

    NUCLEAR PHYSICS TRENDS   1235   219 - +   2010

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    We have searched for a time-modulated decay in a standard electron capture experiment for (140)pr in order to confirm a report from GSI, where an oscillatory decay has been observed for hydrogen-like Pr-140 and Pm-142 ions in the cooler storage ring. Pr-140 has been produced with the Ce-140(p, n) reaction by a pulsed proton beam accelerated from the Van de Graaff accelerator at Osaka University. Resultant time dependence of the k(alpha) and K-beta X-ray intensities from the daughter shows no oscillatory behavior.

    DOI: 10.1063/1.3442597

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  • Electromagnetic Moments of Proton-Rich P-28 and Decomposition of Its Spin Reviewed

    K. Matsuta, Shengyun Zhu, M. Mihara, Dongmei Zhou, D. Nishimura, Yongnan Zheng, M. Fukuda, Daqing Yuan, R. Matsumiya, Yi Zuo, J. Komurasaki, Ping Fan, Xizhen Zhang, D. Ishikawa, T. Suzuki, T. Nagatomo, T. Izumikawa, T. Ohtsubo, S. Takahashi, H. Hirano, Y. Shimbara, T. Kubo, R. Yamada, Y. Namiki, M. Nagashima, S. Momota, K. Ooi, Y. Nojiri, D. Kameda, A. Kitagawa, M. Kanazaw, M. Torikoshi, S. Sato, T. Minamisono, T. Sumikamall, M. Ogura, H. Akai, J. R. Alonso, T. J. M. Symons, G. F. Krebs

    NUCLEAR PHYSICS TRENDS   1235   260 - +   2010

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    The magnetic moment of P-28 (I-pi = 3(+), T-1/2 = 270.3 ms) has been measured precisely by means of beta-NMR technique. The obtained magnetic moment is vertical bar mu(P-28)vertical bar = 0.3115 (34) mu(N). Combined with the magnetic moment of its mirror partner Al-28, the nuclear spin I = 3 is decomposed into its 4 components. The measurement of the Q moment has also been tried. From the preliminary NQR spectrum, it was found that the quadrupole coupling constant eqQ/h may be slightly larger than the prediction, which may show enhancement of the Q moment.

    DOI: 10.1063/1.3442605

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  • Reaction cross sections at intermediate energies and Fermi-motion effect Reviewed

    M. Takechi, M. Fukuda, M. Mihara, K. Tanaka, T. Chinda, T. Matsumasa, M. Nishimoto, R. Matsumiya, Y. Nakashima, H. Matsubara, K. Matsuta, T. Minamisono, T. Ohtsubo, T. Izumikawa, S. Momota, T. Suzuki, T. Yamaguchi, R. Koyama, W. Shinozaki, M. Takahashi, A. Takizawa, T. Matsuyama, S. Nakajima, K. Kobayashi, M. Hosoi, T. Suda, M. Sasaki, S. Sato, M. Kanazawa, A. Kitagawa

    PHYSICAL REVIEW C   79 ( 6 )   2009.6

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    Precise measurements of the reaction cross sections (sigma(R)) for C-12 on Be, C, and Al targets and Be-11 on Be targets were performed in the energy range between 30 and 400 MeV/nucleon. The energy dependencies of sigma(R) for C-12, Be-11, and B-8 were compared to Glauber-type calculations performed using reliable nucleon-density distributions that are supported by experimental data. It was found that the Glauber-type calculations, which include the higher-order multiple scattering effect, the finite-range effect, and the Fermi-motion effect of nucleons in the nucleus, seem to provide a good prescription relating sigma(R) at intermediate energies to a proper nucleon-density distribution. This method provides a powerful tool with which to study the nuclear surface structure through the sigma(R) measurements.</p>.

    DOI: 10.1103/PhysRevC.79.061601

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  • Publisher's Note: Schottky Mass Measurement of the Hg-208 Isotope: Implication for the Proton-Neutron Interaction Strength around Doubly Magic Pb-208 [Phys. Rev. Lett. 102, 122503 (2009)] Reviewed

    L. Chen, Yu. A. Litvinov, W. R. Plass, K. Beckert, P. Beller, F. Bosch, D. Boutin, L. Caceres, R. B. Cakirli, J. J. Carroll, R. F. Casten, R. S. Chakrawarthy, D. M. Cullen, I. J. Cullen, B. Franzke, H. Geissel, J. Gerl, M. Gorska, G. A. Jones, A. Kishada, R. Knoebel, C. Kozhuharov, S. A. Litvinov, Z. Liu, S. Mandal, F. Montes, G. Muenzenberg, F. Nolden, T. Ohtsubo, Z. Patyk, Zs. Podolyak, R. Propri, S. Rigby, N. Saito, T. Saito, C. Scheidenberger, M. Shindo, M. Steck, P. Ugorowski, P. M. Walker, S. Williams, H. Weick, M. Winkler, H. -J. Wollersheim, T. Yamaguchi

    PHYSICAL REVIEW LETTERS   102 ( 13 )   2009.4

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    DOI: 10.1103/PhysRevLett.102.139904

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  • Schottky Mass Measurement of the Hg-208 Isotope: Implication for the Proton-Neutron Interaction Strength around Doubly Magic Pb-208 Reviewed

    L. Chen, Yu. A. Litvinov, W. R. Plass, K. Beckert, P. Beller, F. Bosch, D. Boutin, L. Caceres, R. B. Cakirli, J. J. Carroll, R. F. Casten, R. S. Chakrawarthy, D. M. Cullen, I. J. Cullen, B. Franzke, H. Geissel, J. Gerl, M. Gorska, G. A. Jones, A. Kishada, R. Knoebel, C. Kozhuharov, S. A. Litvinov, Z. Liu, S. Mandal, F. Montes, G. Muenzenberg, F. Nolden, T. Ohtsubo, Z. Patyk, Zs. Podolyak, R. Propri, S. Rigby, N. Saito, T. Saito, C. Scheidenberger, M. Shindo, M. Steck, P. Ugorowski, P. M. Walker, S. Williams, H. Weick, M. Winkler, H. -J. Wollersheim, T. Yamaguchi

    PHYSICAL REVIEW LETTERS   102 ( 12 )   2009.3

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    Time-resolved Schottky mass spectrometry has been applied to uranium projectile fragments which yielded the mass value for the Hg-208 (Z=80, N=128) isotope. The mass excess value of ME=-13 265(31) keV has been obtained, which has been used to determine the proton-neutron interaction strength in Pb-210, as a double difference of atomic masses. The results show a dramatic variation of the strength for lead isotopes when crossing the N=126 neutron shell closure, thus confirming the empirical predictions that this interaction strength is sensitive to the overlap of the wave functions of the last valence neutrons and protons.

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  • Nuclear structure of proton-rich unstable nucleus P-28 studied by g-factor measurement Reviewed

    Zheng Yong-Nan, Zhou Dong-Mei, K. Matsuta, M. Mihara, M. Fukuda, D. Nishimura, J. Komurasaki, D. Ishikawa, R. Matsumiya, T. Nagatomo, T. Izumikawa, S. Takahashi, H. Hirano, T. Ohtsubo, S. Momota, Y. Nojiri, A. Kitagawa, M. Kanazawa, M. Torikoshi, S. Sato, T. Minamisono, J. R. Alonso, G. F. Krebs, T. J. M. Symons, Yuan Da-Qing, Zuo Yi, Fan Ping, T. Suzuki, Zhang Xi-Zhen, Zhu Sheng-Yun

    CHINESE PHYSICS C   33   215 - 217   2009.3

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    Nuclear structure of proton-rich unstable nucleus P-28 has been studied by measuring its g-factor for the first time. The g-factor of P-28 (I-pi = 3(+,) T-1/2 = 270.3 ms) was measured by means of beta-NMR technique combined with the new polarization technique for charge exchange reaction product in the intermediate energy heavy ion collisions. The obtained g-factor of g=0.1028(27) is very much quenched from the Schmidt value. but is well reproduced by the shell model (+0.102). In connection with the magnetic. moment. of the mirror partner and the beta-ray transition probability, the orbital angular momenta and intrinsic spins of protons and neutrons have been determined as < l(p)> = 0.43(29), < l(n)> = 1.85(29), < S-p > = 0.28(4), and < S-n > = 0.44(4).

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  • BEAM OPTICS SIMULATION OF RARE-RI RING AT RI BEAM FACTORY IN RIKEN Reviewed

    I. Arai, A. Ozawa, Y. Yasuda, T. Fujinawa, N. Fukunishi, T. Ohnishi, A. Goto, K. Y. Hara, H. Sakurai, M. Wakasugi, Y. Yamaguchi, Y. Yano, T. Suzuki, T. Yamaguchi, T. Kikuchi, T. Ohtsubo

    INTERNATIONAL JOURNAL OF MODERN PHYSICS E-NUCLEAR PHYSICS   18 ( 2 )   498 - 504   2009.2

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    The cyclotron-like storage ring dedicated to Rare-RI Ring project consists of 6 magnetic sectors and 6 straight sections, having a circumference of 56.13 m. The magnetic sector works for both bending and focusing. The total circulation is assumed to be 1,000 turns. Over the momentum range from 1% to +1% in Delta p/p, the required isochronisity is 10(-6) while the beam emittance is sevaral tens of pi mm-mrad. To examine the design of cyclotron-like storage ring and fix its parameters, we have developed a high precision beam optics simulation. To achieve the precision as high as possible with in a feasible computational time, we have adopted a geometrical tracking assuming a circular orbit for a small spatial segment. For that purpose, it is enough that the magnetic sector is divided into 150 sub-sectors in calculation. In each sub-sector, the magnetic field is given as a function of radial position but uniform around the vicinity of beam trajectory. The beam trajectory is evaluated in 4th order Runge-Kutta algorithm. Finally, we have achieved a precision of 10(-9) in Delta T/T and a computational time of 1.8 sec on atypical PC server for ray tracing of single particle undergoing a circulation of 1,000 turns.

    DOI: 10.1142/S0218301309012550

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  • PRESENT STATUS OF RARE-RI RING PROJECT IN RIKEN RIBF Reviewed

    Y. Yasuda, A. Ozawa, I. Arai, T. Fujinawa, N. Fukunishi, T. Ohnishi, A. Goto, K. Y. Hara, H. Sakurai, M. Wakasugi, Y. Yamaguchi, Y. Yano, T. Suzuki, T. Yamaguchi, T. Kkikuchi, T. Ohtsubo

    INTERNATIONAL JOURNAL OF MODERN PHYSICS E-NUCLEAR PHYSICS   18 ( 2 )   459 - 464   2009.2

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    We are going to construct a precise mass-measurement apparatus; "Rare-RI Ring" at RIKEN RI Beam Factory and measure masses of exotic neutron-rich nuclei far from the stability line with the assistance of high intensity primary beam from the cyclotrons at RIBF. The present status of our project and the progress of some parts of Rare-RI Ring will be presented.

    DOI: 10.1142/S0218301309012501

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  • LARGE-SCALE MASS MEASUREMENTS OF SHORT-LIVED NUCLIDES WITH THE ISOCHRONOUS MASS SPECTROMETRY AT GSI Reviewed

    B. Sun, R. Knoebel, Yu A. Litvinov, S. Nakajima, H. Geissel, J. Meng, K. Beckert, F. Bosch, D. Boutin, C. Brandau, L. Chen, I. J. Cullen, C. Dimopoulou, B. Fabian, M. Hausmann, O. Klepper, C. Kozhuharov, J. Kurcewicz, S. A. Litvinov, M. Mazzocco, F. Montes, G. Muenzenberg, A. Musumarra, C. Nociforo, F. Nolden, T. Ohtsubo, A. Ozawa, Z. Patyk, W. R. Plass, C. Scheidenberger, M. Steck, T. Suzuki, P. M. Walker, H. Weick, N. Winckler, M. Winkler, T. Yamaguchi

    INTERNATIONAL JOURNAL OF MODERN PHYSICS E-NUCLEAR PHYSICS   18 ( 2 )   346 - 351   2009.2

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    Precise mass measurements of short-lived exotic nuclei are very important for the understanding of basic nuclear structure physics and astrophysical nucleosynthesis in nature, as well as for the test and the development of theoretical nuclear mass models. At GSI, the Isochronous Mass Spectrometry (IMS) dedicated to mass measurements of short-lived nuclides was developed. In this contribution, the IMS technique is briefly reviewed. Recently, the first large-scale measurement on the (238)U fission fragment was done successfully. The measured mass values are in excellent agreement with the recent Penning trap data, however, they show a systematical deviation from the values in the latest atomic mass evaluation. Some representative results from this experiment will be presented, including their impact on nuclear structure physics and astrophysical r-process nucleosynthesis.

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  • Electron Screening Effects on alpha-decay Reviewed

    A. Musumarra, F. Farinon, C. Nociforo, H. Geissel, G. Baur, K-H. Behr, A. Bonasera, F. Bosch, D. Boutin, A. Bruenle, L. Chen, A. Del Zoppo, C. Dimopoulou, A. Di Pietro, T. Faestermann, P. Figuera, K. Hagino, R. Janik, C. Karagiannis, P. Kienle, S. Kimura, R. Knoebel, I. Kojouharov, C. Kozhuharov, T. Kuboki, J. Kurcewicz, N. Kurz, K. Langanke, M. Lattuada, S. A. Litvinov, Yu. A. Litvinov, G. Martinez-Pinedo, M. Mazzocco, F. Montes, Y. Motizuki, F. Nolden, T. Ohtsubo, Y. Okuma, Z. Patyk, M. G. Pellegriti, W. Plass, S. Pietri, Z. Podolyak, A. Prochazka, C. Scheidenberger, V. Scuderi, B. Sitar, M. Steck, P. Strmen, B. Sun, T. Suzuki, I. Szarka, D. Torresi, H. Weick, J. S. Winfield, M. Winkler, H. J. Wollersheim, T. Yamaguchi

    NUCLEAR STRUCTURE AND DYNAMICS '09   1165   415 - +   2009

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    An open problem in Nuclear Astrophysics concerns the understanding of electron-screening effects on nuclear reaction rates at stellar energies. In this framework, we have proposed to investigate the influence of the electron cloud on alpha-decay by measuring Q-values and alpha-decay half-lives of fully stripped, H-like and He-like ions. These kinds of measurements have been feasible just recently for highly-charged radioactive nuclides by fragmentation of U-238 at relativistic energies at the FRS-ESR facility at GSI. In this way it is possible to produce, efficiently separate and store highly-charged alpha-emitters. Candidates for the proposed investigation were carefully selected and will be studied by using the Schottky Mass Spectroscopy technique.
    In order to establish a solid reference data set, lifetimes and Q(alpha)-value measurements of the corresponding neutrals have been performed directly at the FRS, by implanting the separated ions into an active Silicon stopper.

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  • Measurement of the reaction cross section of (18)C and observations of fragments from (17)C and (18)C at 80A MeV Reviewed

    A. Ozawa, D. Q. Fang, M. Fukuda, N. Iwasa, T. Izumikawa, H. Jeppesen, R. Kanungo, R. Koyama, T. Ohnishi, T. Ohtsubo, W. Shinozaki, T. Suda, T. Suzuki, M. Takahashi, I. Tanihata, C. Wu, Y. Yamaguchi

    PHYSICAL REVIEW C   78 ( 5 )   2008.11

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    The one- and two-neutron removal reactions from (17)C and (18)C as well as the reaction cross section of (18)C have been studied using a carbon target at 80A MeV. The longitudinal momentum distributions of (15,16)C fragments from (17)C and (16,17)C fragments from (18)C were measured by a direct time-of-flight method. The width of (15)C fragments from (17)C is fairly smaller than that from other C isotopes. The experimental data are discussed within the framework of the Glauber model.

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  • Nuclear structure studies of short-lived neutron-rich nuclei with the novel large-scale isochronous mass spectrometry at the FRS-ESR facility Reviewed

    B. Sun, R. Knoebel, Yu. A. Litvinov, H. Geissel, J. Meng, K. Beckert, F. Bosch, D. Boutin, C. Brandau, L. Chen, I. J. Cullen, C. Dimopoulou, B. Fabian, M. Hausmann, C. Kozhuharov, S. A. Litvinov, M. Mazzocco, F. Montes, G. Muenzenberg, A. Musumarra, S. Nakajima, C. Nociforo, F. Nolden, T. Ohtsubo, A. Ozawa, Z. Patyk, W. R. Plass, C. Scheidenberger, M. Steck, T. Suzuki, P. M. Walker, H. Weick, N. Winckler, M. Winkler, T. Yamaguchi

    NUCLEAR PHYSICS A   812   1 - 12   2008.11

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    The previously pioneered Isochronous Mass Spectrometry (IMS) has been extended by an additional precise magnetic-rigidity determination to enable accurate large-scale measurements of stored short-lived relativistic nuclei with the FRS-ESR facility at 382 MeV/u. With this novel experimental tool the mass resolving power and accuracy have been improved by a factor of about 3. The recorded broad-band revolution time spectrum corresponds to the mass-over-charge range of about 6%. A mass resolving power of 200 000 (FWHM) and a typical accuracy of 120 keV have been achieved almost over the entire spectrum. The masses of 35 neutron-rich nuclides have been directly measured in the element range from aluminum to barium. The Masses of 8 nuclides (As-85,As-86, Se-89, Ag-123, Te-138, I-140,I-141, Xe-143) have been measured for the first time. The results are compared with previous experimental data and theoretical predictions. The evolution of the N = 50 shell closure towards doubly-magic Ni-78 is discussed. (c) 2008 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nuclphysa.2008.08.013

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  • Studies on the exotic structure of Al-23 Reviewed

    Fang De-Qing, Guo Wei, Ma Chun-Wang, Wang Kun, Yan Ting-Zhi, Ma Yu-Gang, Cai Xiang-Zhou, Shen Wen-Qing, Ren Zhong-Zhou, Sun Zhi-Yu, M. Hosoi, T. Izumikawa, R. Kanungo, S. Nakajima, T. Ohnishi, T. Ohtsubo, A. Ozawa, T. Suda, K. Sugawara, T. Suzuki, A. Takisawa, K. Tanaka, T. Yamaguchi, I. Tanihata

    CHINESE PHYSICS C   32   34 - 37   2008.10

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    The longitudinal momentum distribution (P-//) of fragments after one-proton removal from Al-23 and reaction cross sections (sigma(R)) for Al-23,Al-24 on carbon target at 74A MeV have been measured simultaneously. An enhancement in sigma(R) is observed for Al-23 compaxed with Al-24. The full width at half maximum of the P-// distribution for Mg-22 fragments has been determined to be 232 +/- 28 MeV/c. Analysis of P-// using the Few-Body Glauber Model indicates a dominant d-wave configuration for the valence proton in the ground state of Al-23. The exotic structure in Al-23 is discussed.

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  • Development of a time-of-flight detector for the Rare-RI Ring project at RIKEN Reviewed

    S. Nakajima, T. Kuboki, M. Yoshitake, Y. Hashizume, M. Kanazawa, A. Kitagawa, K. Kobayashi, T. Moriguchi, T. Ohtsubo, A. Ozawa, S. Sato, T. Suzuki, Y. Yamaguchi, Y. Yasuda, T. Yamaguchi

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B-BEAM INTERACTIONS WITH MATERIALS AND ATOMS   266 ( 19-20 )   4621 - 4624   2008.10

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    We have tested the timing properties of several thin plastic scintillators (10-500 mu m) designed for the Rare-RI Ring project at the R I beam factory. The experiments were performed at the heavy-ion synchrotron facility, HIMAC (Heavy Ion Medical Accelerator in Chiba), using a Xe beam with an energy of 200 MeV/nucleon. The scintillation light was read Out by fast-timing photomultipliers through standard fishtail-shaped light guides. The resultant timing resolutions reached a few tens of picoseconds, which satisfied our requirement for the project. We also measured charge-state distributions for Xe42+ and Fe20+ ions penetrating carbon foils of 10-500 mu g/cm(2) thickness. The results were compared with a theoretical model calculation for charge-state evolution. (c) 2008 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nimb.2008.05.085

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  • Rare-RI ring project at RIKEN RI beam factory Reviewed

    Y. Yamaguchi, A. Ozawa, A. Goto, I. Arai, T. Fujinawa, N. Fukunishi, T. Kikuchi, T. Ohnishi, T. Ohtsubo, H. Sakurai, T. Suzuki, M. Wakasugi, T. Yamaguchi, Y. Yasuda, Y. Yano

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B-BEAM INTERACTIONS WITH MATERIALS AND ATOMS   266 ( 19-20 )   4575 - 4578   2008.10

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    A new apparatus named "Rare-RI Ring", for precisely measuring the masses of short-lived rare nuclei including the r-process region is proposed. The Rare-RI Ring is one of the major experimental installations at the RI KEN RI beam Factory. It consists of three main parts: a long injection beam line, a fast kicker system and a cyclotron-like storage ring. The combination of a long injection beam line and a feast kicker system enables Lis to inject short-lived rare nuclei into the ring one by one. The revolution time of each nucleus in the ring is measured with all accuracy of better than 10(-6). Overall, the masses of short-lived rare nuclei including the r-process region can be determined with an order of 10(-6) precision. (c) 2008 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nimb.2008.05.081

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  • Nuclear matter radii of neutron-deficient Kr isotopes Reviewed

    T. Yamaguchi, T. Suzuki, T. Ohnishi, F. Becker, M. Fukuda, H. Geissel, M. Hosoi, R. Janik, K. Kimura, T. Kuboki, S. Mandel, M. Matsuo, G. Muenzenberg, S. Nakajima, T. Ohtsubo, A. Ozawa, A. Prochazka, M. Shindo, B. Sitar, P. Strmen, T. Suda, K. Suemmerer, K. Sugawara, I. Szarka, M. Takechi, A. Takisawa, K. Tanaka, M. Yamagami

    PHYSICAL REVIEW C   77 ( 3 )   2008.3

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    Interaction cross sections (sigma(I)) of Kr-72,Kr-76,Kr-80 on a C target were measured at the projectile fragment separator FRS at GSI. Effective matter radii of the nuclei were deduced by a Glauber model analysis so as to reproduce the experimental sigma(I). An increase of matter radii toward the proton drip-line is observed. We compare the extracted radii to theoretical predictions, which are based on Skyrme-Hartree-Fock-Bogoliubov (SHFB) and on relativistic mean field (RMF) approaches. The enhancement of the matter radius observed in Kr-72 is discussed.

    DOI: 10.1103/PhysRevC.77.034315

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  • New scheme for precision mass measurements of rare isotopes produced at RI beam factory Reviewed

    S. Nakajima, T. Yamaguchi, T. Suzuki, Y. Yamaguchi, T. Fujinawa, N. Fukunishi, A. Goto, T. Ohnishi, H. Sakurai, M. Wakasugi, Y. Yano, I. Arai, A. Ozawa, Y. Yasuda, T. Kikuchi, T. Ohtsubo

    ACTA PHYSICA POLONICA B   39 ( 2 )   457 - 462   2008.2

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    For precision mass measurements of short-lived rare isotopes, a new experimental apparatus, named "Rare-RI Ring", has recently been proposed. A unique possibility of the project is discussed, comparing with other experimental techniques. The current status is presented.

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  • SIGNALS OF ENLARGED CORE IN (23)AL Reviewed

    Y. G. Ma, D. Q. Fang, C. W. Ma, K. Wang, T. Z. Yan, X. Z. Cai, W. Q. Shen, Z. Y. Sun, Z. Z. Ren, J. G. Chen, J. H. Chen, G. H. Liu, E. J. Ma, G. L. Ma, Y. Shi, Q. M. Su, W. D. Tian, H. W. Wang, C. Zhong, J. X. Zuo, M. Hosoi, T. Izumikawa, R. Kanungo, S. Nakajima, T. Ohnishi, T. Ohtsubo, A. Ozawa, T. Suba, K. Sugawara, K. Suzuki, A. Takisawa, K. Tanaka, T. Yamaguchi, I. Tanihata

    DYNAMICAL ASPECTS OF NUCLEAR FISSION   191 - +   2008

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    The longitudinal momentum distribution (P-parallel to) of fragments after one-proton removal from Al-23 and reaction cross sections (sigma(R)) for Al-23,Al-24 on carbon target at 74AMeV have been measured using 135AMeV Si-28 primary beam on RIPS in RIKEN. P-parallel to is measured by a direct time-of-flight (TOF) technique, while sigma(R) is determined using a transmission method. An enhancement in sigma(R) is observed for Al-23 compared with Al-24. The P-parallel to for Mg-22 fragments from Al-23 breakup has been obtained for the first time. FWHM of the distributions has been determined to be 233 +/- 14 MeV/c. The experimental data are discussed by use of the Few-Body Glauber Model (FBGM). Analysis of P indicates a dominant d-wave configuration for the valence proton in the ground state of Al-23. The possibility of an enlarged Mg-22 core for proton-rich nucleus Al-23 is demonstrated..

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  • Magnetic moment of short lived beta-emitter (24m)Al Reviewed

    D. Nishimura, J. Komurasaki, K. Matsuta, M. Mihara, R. Matsumiya, S. Momota, T. Ohtsubo, T. Izumikawa, H. Hirano, A. Kitagawa, M. Kanazawa, M. Torikoshi, S. Sato, M. Fukuda, D. Ishikawa, T. Minamisono, R. Watanabe, T. Kubo, Y. Nojiri, J. R. Alonso, G. F. Krebs, T. J. M. Symons

    HYPERFINE INTERACTIONS   180 ( 1-3 )   71 - 74   2007.11

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    The magnetic moment of short lived beta-emitter (24m)Al (426 keV, I(pi) = 1(+), T(1/2) = 131 ms) has been measured by means of beta-NMR technique, for the first time. From the beta-NMR spectrum, the magnetic moment was determined as vertical bar mu((24m)Al)vertical bar = (2.99 +/- 0.09) mu(N). Combined with the known magnetic moment of the mirror partner (24m)Na, the expectation value of <S(z)> is obtained to be (0.08 +/- 0.12). These values are reproduced well by the shell model calculation.

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  • Nuclear radius systematics of Kr isotopes studied via their interaction cross-sections at relativistic energies Reviewed

    T. Yamaguchi, T. Suzuki, T. Ohnishi, K. Suemmerer, F. Becker, M. Fukuda, H. Geissel, M. Hosoi, R. Janik, K. Kimura, S. Mandal, G. Muenzenberg, S. Nakajima, T. Ohtsubo, A. Ozawa, A. Prochazka, M. Shindo, B. Sitar, P. Strmen, T. Suda, K. Sugawara, I. Szarka, A. Takisawa, M. Takechi, K. Tanaka

    EUROPEAN PHYSICAL JOURNAL-SPECIAL TOPICS   150   197 - 200   2007.11

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    The interaction cross-sections of neutron-deficient Kr-72,Kr-76,Kr-80 isotopes have been measured by use of the transmission method at relativistic energies. Based on the Glauber model analysis effective root-mean-square matter radii of these nuclei have been determined for the first time. A systematic evolution of the matter radii in the mass A similar to 70 region is discussed and compared with that of light nuclei.

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  • Polarization of Ne-23, Al-24m,Al-25 and P-28 produced through single nucleon pickup and charge-exchange reactions at 100 AMeV Reviewed

    T. Ohtsubo, H. Hirano, S. Takahashi, K. Matsuta, M. Mihara, M. Fukuda, T. Nagatomo, T. Izumikawa, S. Momota, D. Nishimura, J. Komurasaki, D. Ishikawa, D. M. Zhou, Y. N. Zheng, S. Y. Zhu, A. Kitagawa, M. Kanazawa, M. Torikoshi, S. Sato, T. Minamisono, Y. Nojiri, R. Matsumiya, T. Sumikama, K. Tanaka, K. Yamada, A. Ozawa, T. Suzuki, T. Yamaguchi, S. Nakajima, K. Yoshida, Y. Nakashima, H. Fujiwara, S. Kumashiro, M. Ota, D. Shinojima, H. Tanaka, T. Yasuno, K. Muranaka, T. Maemura, A. Chiba, S. A. Pahlovy, M. Nagao, R. Watanabe, T. Kubo, I. Tanihata, M. Takechi, K. Minamisono, J. R. Alonso, G. F. Krebs, T. J. M. Symons

    HYPERFINE INTERACTIONS   180 ( 1-3 )   85 - 89   2007.11

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    We measured the polarization of the beta-emitting Ne-23 (I-pi = 5/2(+), T-1/2 = 37.24 s) and Al-25(I-pi = 5/2(+), T-1/2 = 7.18 s) produced through the one nucleon pickup reactions and Al-24m(I-pi = 1(+), T-1/2 = 131 ms, E-ex = 426 keV) and P-28(I-pi = 3(+), T-1/2 = 270 ms) produced through charge-exchange reactions in the intermediate energy heavy ion collisions. We compared them with those from the projectile fragmentation process. The larger polarization seems to persistently be positive throughout the momentum distribution, and sharper momentum distributions suggest that nuclear friction mechanism is responsible for the polarization phenomena.

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  • Hyperfine anomalies of Sc isotopes (A=44, 44 m, 46 and 47) in iron Reviewed

    S. Ohya, T. Ohtsubo, T. Izumikawa, K. Nishimura, S. Muto, T. Shinozuka

    HYPERFINE INTERACTIONS   180 ( 1-3 )   55 - 60   2007.11

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    Nuclear magnetic resonance on oriented nuclei (NMR-ON) on Sc isotopes (A = 44, 44 m, 46, 47) in Fe were performed. Using the known magnetic moments the magnetic hyperfine fields were determined. The hyperfine anomalies of various Sc were deduced; (44)Delta(47) = 0.0 (12) %, (44)m Delta(47) = 1.2 (4) %, (46)Delta(47) = 2.7 (8) %. The measured hyperfine anomalies are briefly discussed based on the shell model.

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  • Magnetic moment of (48)Sc Reviewed

    T. Ohtsubo, Y. Kawamura, S. Ohya, T. Izumikawa, K. Nishimura, S. Muto, T. Shinozuka

    HYPERFINE INTERACTIONS   180 ( 1-3 )   79 - 83   2007.11

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    Nuclear magnetic resonances were measured for (48)Sc and (44m)Sc oriented at 8 mK in an Fe host metal. The magnetic hyperfine splitting frequencies at an external magnetic field of 0.2 T were determined to be 63.22(11) MHz and 64.81(1) MHz for (48)Sc and (44m)Sc, respectively. With the known magnetic moment of mu((44m)Sc) = + 3.88 (1) mu(N), the magnetic moment of (48)Sc is deduced as vertical bar mu((48)Sc)vertical bar = 3.785 (12) mu(N). The measured magnetic moment of (48)Sc is discussed in terms of the shell model using the effective interactions.

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  • Magnetic moment of proton halo nucleus (28)P Reviewed

    Dongmei Zhou, Yongnan Zheng, K. Matsuta, M. Mihara, M. Fukuda, D. Nishimura, J. Komurasaki, D. Ishikawa, R. Matsumiya, T. Nagatomo, T. Izumikawa, S. Takahashi, H. Hirano, T. Ohtsubo, S. Momota, Y. Nojiri, A. Kitagawa, M. Kanazawa, M. Torikoshi, S. Sato, T. Minamisono, J. R. Alonso, G. F. Krebs, T. J. M. Symons, Daqing Yuan, Yi Zuo, Ping Fan, T. Suzuki, Xizhen Zhang, Shengyun Zhu

    HYPERFINE INTERACTIONS   180 ( 1-3 )   37 - 42   2007.11

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    The magnetic moment of (28)P (I(pi) = 3(+), T(1/2) = 270.3 ms) in the ground state has been measured by the beta-nuclear magnetic resonance method for the first time. The measured magnetic moment of vertical bar mu((28)P)vertical bar = 0.309( 9) mu(N) is well reproduced by the shell model value of +0.306 mu(N). The shell model calculation also yields a proton density distribution with a long tail. The present results provide a strong confirmation of the configuration of the 2s(1/2) proton which should lead to the proton halo.

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  • Hyperfine interaction of Al-25 in alpha-Al2O3 and its quadrupole moment Reviewed

    K. Matsuta, M. Mihara, T. Nagatomo, R. Matsumiya, S. Momota, T. Ohtsubo, T. Izumikawa, H. Hirano, S. Takahashi, D. Nishimura, J. Komurasaki, A. Kitagawa, M. Kanazawa, M. Torikoshi, S. Sato, M. Fukuda, T. Minamisono, T. Sumikama, K. Tanaka, M. Takechi, D. Ishikawa, S. A. Pahlovy, M. Nagao, Y. Nojiri, J. R. Alonso, G. F. Krebs, T. J. M. Symons

    HYPERFINE INTERACTIONS   180 ( 1-3 )   65 - 69   2007.11

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    The electric quadrupole (Q) moment of short-lived nucleus Al-25 (I-pi = 5/2(+), T-1/2 = 7.18 s) has been measured for the first time, by means of the beta-NQR technique. The spin polarization of Al-25 was produced in heavy ion collisions and was kept in a alpha-Al2O3 single crystal for as long as 2 s and the quadrupole coupling frequency was obtained as vertical bar eqQ/h(Al-25 in Al2O3)vertical bar = (4.05 +/- 0.30) MHz. From the result, the Q moment was determined as vertical bar Q(Al-25)vertical bar = (240 +/- 20) mb. The present

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  • Examining the exotic structure of the proton-rich nucleus Al-23 Reviewed

    D. Q. Fang, W. Guo, C. W. Ma, K. Wang, T. Z. Yan, Y. G. Ma, X. Z. Cai, W. Q. Shen, Z. Z. Ren, Z. Y. Sun, J. G. Chen, W. D. Tian, C. Zhong, M. Hosoi, T. Izumikawa, R. Kanungo, S. Nakajima, T. Ohnishi, T. Ohtsubo, A. Ozawa, T. Suda, K. Sugawara, T. Suzuki, A. Takisawa, K. Tanaka, T. Yamaguchi, I. Tanihata

    PHYSICAL REVIEW C   76 ( 3 )   2007.9

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    The longitudinal momentum distribution (P-//) of fragments after one-proton removal from Al-23 and reaction cross sections (sigma(R)) for Al-23,Al-24 on a carbon target at 74A MeV have been measured. The Al-23,Al-24 ions were produced through projectile fragmentation of 135A MeV Si-28 primary beam using the RIPS fragment separator at RIKEN. P-// is measured by a direct time-of-flight (TOF) technique, while sigma(R) is determined using a transmission method. An enhancement in sigma(R) is observed for Al-23 compared with Al-24. The P-// for Mg-22 fragments from Al-23 breakup has been obtained for the first time. FWHM of the distributions has been determined to be 232 +/- 28 MeV/c. The experimental data are discussed by using the Few-Body Glauber model. Analysis of P-// demonstrates a dominant d-wave configuration for the valence proton in ground state of Al-23, indicating that Al-23 is not a proton halo nucleus.

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  • Temperature dependence of the lattice locations of boron implanted in germanium Reviewed

    T. Izumikawa, D. Shinojima, S. Takahashi, M. Mihara, K. Matsuta, M. Fukuda, T. Ohtsubo, S. Ohya, T. Minamisono

    HYPERFINE INTERACTIONS   178 ( 1-3 )   79 - 82   2007.7

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    The beta-NMR of the probe atom (12)B implanted in In-doped germanium was measured as a function of temperature. As a result, three resonances were observed: sharp and broad resonances around the Larmor frequency and a resonance split by the electric quadrupole interaction. It was found that the appearance of the resonances is similar to the case of Si host (Izumikawa et al. Hyperfine Interact. 136/137:559-605, 2001). The quadrupole coupling constant for the split resonance was deduced as vertical bar eqQ/h vertical bar = 252(3) kHz under the assumption that it has < 111 > axial symmetry. And furthermore, assuming that the defect atom jumps thermally between the identical defect sites, the activation energy of the jump was deduced as 0.4 +/- 0.1 eV.

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  • Spin-lattice relaxation of Al-25 and P-28 in Pt Reviewed

    M. Mihara, K. Matsuta, D. Nishimura, T. Nagatomo, R. Matsumiya, S. Momota, T. Ohtsubo, T. Izumikawa, D. M. Zhou, Y. N. Zheng, M. Ogura, H. Akai, J. Komurasaki, M. Fukuda, D. Ishikawa, Y. Nojiri, H. Hirano, S. Takahashi, R. Watanabe, T. Kubo, S. Y. Zhu, A. Kitagawa, M. Kanazawa, S. Sato, M. Torikoshi, T. Sumikama, T. Minamisono, J. R. Alonso, G. F. Krebs, T. J. M. Symons

    HYPERFINE INTERACTIONS   178 ( 1-3 )   83 - 86   2007.7

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    The spin-lattice relaxation times T-1 for short-lived beta emitters Al-25(I = 5/2, T-1/ 2 = 7.2 s) and P-28(I = 3, T-1/2 = 270 ms) in Pt were measured by means of the beta-NMR technique. As a result, T-1[Al-25 in Pt] = (1.1(- 0.3)(+0.7)) s and T-1[P-28 in Pt] > 0.5 s were obtained at temperatures of 17 and 20 K, respectively. The Knight shifts were estimated from the Korringa relation, which were evaluated by comparing to the first principle calculations.

    DOI: 10.1007/s10751-008-9662-4

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  • Status of the experimental program on mass measurements of stored exotic nuclei at the FRS-ESR facility Reviewed

    Yu A. Litvinov, H. Geissel, K. Beckert, P. Beller, F. Bosch, D. Boutin, C. Brandau, L. Chen, I. Cullen, C. Dimopoulou, B. Fabian, M. Hausmann, O. Klepper, R. Knoebel, C. Kozhuharov, J. Kurcewicz, S. A. Litvinov, Z. Liu, M. Mazzocco, F. Montes, G. Muenzenberg, A. Musumarra, S. Nakajima, C. Nociforo, F. Nolden, T. Ohtsubo, A. Ozawa, Z. Patyk, W. Plass, C. Scheidenberger, M. Steck, B. Sun, T. Suzuki, P. M. Walker, H. Weick, C. Scheidenberger, M. Steck, B. Sun, T. Suzuki, P. M. Walker, H. Weick, N. Winckler, M. Winckler, T. Yamaguchi

    NUCLEAR PHYSICS A   787   315C - 320C   2007.5

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    Schottky Mass Spectrometry (SMS) and Isochronous Mass Spectrometry (IMS) have been successfully applied for direct mass measurements of exotic nuclides at FRS-ESR facility at GSI. Both experimental methods are sensitive to single stored ions and can cover very efficiently a large number of nuclides in one run. Presently, more than 1100 masses of different nuclides have been covered by SMS and IMS in several FRS-ESR experiments whereby about 350 of them have been determined for the first time. In this paper, we present the status of our experimental program and use the experimental mass values to test the predictive power of modern mass models.

    DOI: 10.1016/j.nuclphysa.2006.12.050

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  • Nuclear radii of neutron-deficient Kr isotopes studied via their interaction cross-sections at relativistic energies Reviewed

    T. Yamaguchi, T. Suzuki, T. Ohnishi, K. Suemmerer, F. Becker, M. Fukuda, H. Geissel, M. Hosoi, R. Janik, K. Kimura, S. Mandal, G. Muenzenberg, S. Nakajima, T. Ohtsubo, A. Ozawa, A. Prochazka, M. Shindo, B. Sitar, P. Strmen, T. Suda, K. Sugawara, I. Szarka, A. Takisawa, M. Takechi, K. Tanaka

    NUCLEAR PHYSICS A   787   471C - 475C   2007.5

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    Interaction cross-sections of Kr-72,Kr-76,Kr-80 on a C target were measured at the projectile fragment separator FRS at GSI. We deduced the effective matter radii of the nuclei by a Glauber model analysis. An increase of matter radii toward the proton drip-line was observed.

    DOI: 10.1016/j.nuclphysa.2006.12.070

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  • Proton skin in neutron-deficient nuclei studied via interaction cross-sections at relativistic energies Reviewed

    S. Nakajima, T. Yamaguchi, T. Ohtsubo, A. Ozawa, T. Suzuki

    PROTON EMITTING NUCLEI AND RELATED TOPICS   961   175 - +   2007

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    The interaction cross-sections of neutron-deficient Ar and Kr isotopes were precisely measured using the fragment separator FRS at relativistic energies. Based on Glauber model analysis, effective root-mean-square matter radii of these nuclei were determined. Using charge radii obtained from isotope-shift measurements, an evolution of proton skins for Ar isotopes is clearly shown. A systematics of the matter radii in the mass region A similar to 70 is also discussed.

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  • New study of reaction cross sections and the nucleon density distribution Reviewed

    M. Fukuda, M. Takechi, M. Mihara, R. Matsumiya, K. Matsuta, T. Minamisono, T. Ohtsubo, T. Izumikawa, S. Momota, T. Suzuki, T. Yamaguchi, S. Nakajima, K. Kobayashi, K. Tanaka, T. Suda, S. Sato, M. Kanazawa, A. Kitagawa

    TOURS SYMPOSIUM ON NUCLEAR PHYSICS VI   891   181 - +   2007

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    Reaction cross sections (sigma R) for C-12 beam on Be-9, 12C, and Al-27 targets and for Be-11 beam on 9Be target were precisely measured systematically in the intermediate energy range. It is indicated that these all sigma(R) data were successfully reproduced by a modified Glauber calculation, which is expected to be applied for the determination of density distributions of other exotic nuclei.

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  • Precise studies of nucleon density distribution of He-6 and He-8 Reviewed

    M. Takechi, M. Fukuda, M. Mihara, R. Matsumiya, K. Matsuta, T. Minamisono, T. Ohtsubo, T. Izumikawa, S. Momota, T. Suzuki, T. Yamaguchi, S. Nakajima, K. Kobayashi, K. Tanaka, T. Suda, S. Sato, M. Kanazawa, A. Kitagawa

    TOURS SYMPOSIUM ON NUCLEAR PHYSICS VI   891   187 - +   2007

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    Reaction cross sections (sigma(R)) for He-6 and He-8 have been measured on Be-9, C-12, and Al-27 targets at intermediate energies. We deduced the nucleon density distribution of He-6 and He-8 through our data with the use of modified Glauber calculation. This method is a sensitive probe for dilute nucleon density and we successfully clarified the halo structure of He-6 and the neutron skin-type density distribution of He-8.

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  • Polarization and momentum distribution of Ne-23 and Al-25 produced in one nucleon pickup reactions at 100A MeV Reviewed

    K. Matsuta, T. Nagatomo, M. Mihara, R. Matsumiya, S. Momota, T. Ohtsubo, T. Izumikawa, H. Hirano, S. Takahashi, A. Kitagawa, M. Kanazawa, M. Torikoshi, S. Sato, M. Fukuda, T. Minamisono, A. Ozawa, K. Yamada, T. Suzuki, T. Yamaguchi, S. Nakajima, T. Sumikama, K. Tanaka, K. Yoshida, Y. Nakashima, H. Fujiwara, S. Kumashiro, M. Ota, D. Shinojima, H. Tanaka, T. Yasuno, K. Muranaka, T. Maemura, A. Chiba, S. A. Pahlovy, M. Nagao, I. Tanihata, K. Minamisono, Y. Nojiri, J. R. Alonso, G. F. Krebs, T. J. M. Symons

    PROCEEDINGS OF THE 17TH INTERNATIONAL SPIN PHYSICS SYMPOSIUM   915   837 - +   2007

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    We measured the polarization of the beta-emitting Ne-23 (I-pi = 5/2(+), T-1/2 = 37.24 s) and 25Al(I-pi = 5/2(+), T-1/2 = 7.18 s), produced through the one nucleon pickup reactions in the intermediate energy heavy ion collisions, and was compared with those from the projectile fragmentation process. The larger polarization which seems to persistently be positive throughout the momentum distribution, and sharper momentum distributions suggest nuclear friction mechanism to be responsible for the polarization phenomena. Using such a large polarization, magnetic moment of 23Ne and the quadrupole moment of 25AI were measured. The obtained values are vertical bar mu(Ne-23)vertical bar = 1.0817(9),mu(N) and vertical bar Q(Al-25)vertical bar = (240 +/- 20) mb.

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  • New developments for isochronous mass measurements of short-lived nuclei Reviewed

    R. Knoebel, S. A. Litvinov, B. Sun, K. Beckert, P. Beller, F. Bosch, D. Boutin, C. Brandau, L. Chen, I. J. Cullen, C. Dimopoulou, A. Dolinskii, B. Fabian, H. Geissel, M. Hausmann, C. Kozhuharov, J. Kurcewicz, Yu. A. Litvinov, Z. Liu, M. Mazzocco, F. Montes, G. Muenzenberg, A. Musumarra, S. Nakajima, C. Nociforo, F. Nolden, T. Ohtsubo, A. Ozawa, Z. Patyk, W. R. Plass, C. Scheidenberger, M. Shindo, M. Steck, T. Suzuki, P. M. Walker, H. Weick, N. Winckler, M. Winkler, T. Yamaguchi

    TOURS SYMPOSIUM ON NUCLEAR PHYSICS VI   891   199 - +   2007

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    The combination of the in-flight separator FRS and the storage-ring ESR at GSI offers unique possibilities for high accuracy mass and lifetime measurements of bare and few-electron fragments. Operating the ESR in the isochronous mode allows for measurements of revolution frequencies of stored ions without cooling. Isochronous Mass Spectrometry (IMS) can be applied to fragments with half-lives as short as several tens of microseconds. Newly developed magnetic rigidity tagging increases the resolving power of IMS to about 500000. IMS can be used to measure masses of nuclei with rates even lower than one ion per day, a property also needed for the purpose of the ILIMA project at the future facility FAIR.

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  • Study of exoticness of proton-rich nuclei Al-23 and it's neighboring nuclei Reviewed

    Ma Chun-Wang, Fang De-Qing, Guo Wei, Wang Kun, Yan Ting-Zhi, Ma Yu-Gang, Cai Xiang-Zhou, Shen Wen-Qing, Sun Zhi-Yu, Ren Zhong-Zhou, Chen Jin-Gen, Tian Wen-Dong, Wang Hong-Wei, Ma Er-Jun, Liu Gui-Hua, Shi Yu, Su Qian-Min, Zhong Chen, M. Hosoi, T. Izumikawa, R. Kanungo, S. Nakajima, T. Ohnishi, T. Ohtsubo, T. Suda, K. Sugawara, T. Suzuki, A. Ozawa, A. Takisawa, K. Tanaka, T. Yamaguchi, I. Tanihata

    HIGH ENERGY PHYSICS AND NUCLEAR PHYSICS-CHINESE EDITION   30   186 - 188   2006.12

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    We measured the reaction cross sections(sigma(R)) and parallel momentum distributions(P-//) of Al-23 and it's neighboring nuclei at RIKEN-RIPS. An enhanced sigma(R) of Al-23 is observed, which is consistent with the previous experimental result. And the P-// of fragment from the projectile breakup nuclei have been obtained at the same time. We discuss our experimental data under the Few-Body Glauber Model. The P-// of Al-23 shows the ground state of the valence proton is a d-wave, which is consistent with the recent measurement of Al-23's g factor. To explain the experimental sigma(R) and P-// of Al-23 at the same time, we suggest an enlarged core of Al-23.

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  • Measurements of reaction cross section and fragment momentum distribution for N=10 proton-rich isotones Reviewed

    W. Guo, D. Q. Fang, Y. G. Ma, C. W. Ma, K. Wang, T. Z. Yan, X. Z. Cai, W. Q. Shen, Z. Y. Sun, Z. Z. Ren, J. G. Chen, J. H. Chen, G. H. Liu, E. J. Ma, G. L. Ma, Y. Shi, Q. M. Su, W. D. Tian, H. W. Wang, C. Zhong, J. X. Zuo, M. Hosoi, T. Izumikawa, R. Kanungo, S. Nakajima, T. Ohnishi, T. Ohtsubo, A. Ozawa, T. Suda, K. Sugawara, T. Suzuki, A. Takisawa, K. Tanaka, T. Yamaguchi, I. Tanihata

    INTERNATIONAL JOURNAL OF MODERN PHYSICS E-NUCLEAR PHYSICS   15 ( 7 )   1523 - 1530   2006.10

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    The longitudinal momentum (p(//)) distributions of fragments after one-proton removal and reaction cross sections (sigma R) for several N = 10 isotones at intermediate energy (similar to 70A MeV) have been measured simultaneously at the RIken Projectile fragment Separator (RIPS). p(//) was measured using a direct time-of-flight (TOF) technique, while sigma(R) was determined using a transmission method. An enhanced sigma(R) is observed for Al-23 comparing with its neighbors. The p(//) distribution for Mg-22 fragments from Al-23 one-proton removal reaction has been obtained for the first time. The experimental data are discussed within a Few Body Glauber (FBG) framework. Analysis of p// indicates a dominant d-wave component in the ground state of Al-23. This agrees with recent experimental results. We also suggest the possibility of an enlarged Mg-22 core for proton-rich nucleus Al-23.

    DOI: 10.1142/S0218301306005101

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  • Production cross sections of isotopes formed by fragmentation of similar to 1A (GeVKr)-Kr-80 beam Reviewed

    T. Yamaguchi, T. Ohnishi, T. Suzuki, F. Becker, M. Fukuda, H. Geissel, M. Hosoi, R. Janik, A. Kelic, K. Kimura, S. Mandel, G. Muenzenberg, S. Nakajima, T. Ohtsubo, A. Ozawa, A. Prochazka, M. Shindo, B. Sitar, P. Strmen, T. Suda, K. Summerer, K. Sugawara, I. Szarka, M. Takechi, A. Takisawa, K. Tanaka

    PHYSICAL REVIEW C   74 ( 4 )   2006.10

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    Production cross sections for the projectile fragmentation of a 1.05A GeV Kr-80 beam on a Be target were measured at the projectile fragment separator FRS at GSI. Cross sections were obtained for isotopes of the elements Ge to Kr close to the proton drip line. These data are compared to the results of the empirical parametrization EPAX and to abrasion-ablation calculations. We also compare the results to predictions of intranuclear-cascade calculations. The intranuclear-cascade calculations allow us to also compare well measured one-proton pickup cross sections.

    DOI: 10.1103/PhysRevC.74.044608

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  • Measurement of the spin and magnetic moment of Al-23 Reviewed

    A. Ozawa, K. Matsuta, T. Nagatomo, M. Mihara, K. Yamada, T. Yamaguchi, T. Ohtsubo, S. Momota, T. Izumikawa, T. Sumikama, Y. Nakashima, H. Fujiwara, S. Kumashiro, R. Matsumiya, M. Ota, D. Shinojima, H. Tanaka, T. Yasuno, S. Nakajima, T. Suzuki, K. Yoshida, K. Muranaka, T. Maemura, A. Chiba, Y. Utsuno, M. Fukuda, K. Tanaka, I. Tanihata, Y. Nojiri, T. Minamisono, J. R. Alonso, G. F. Krebs, T. J. M. Symons

    PHYSICAL REVIEW C   74 ( 2 )   2006.8

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    For the first time, we obtained the g factor for the ground state of Al-23 by use of a beta-NMR measurement. Al-23 has a small proton separation energy and is a potential proton-halo candidate. The obtained g factor, vertical bar g vertical bar=1.557 +/- 0.088, clearly shows the spin and parity, J(pi)=5/2(+), for Al-23, which is the same as that of its mirror partner, Ne-23. The possible nuclear structure of Al-23 is also discussed.

    DOI: 10.1103/PhysRevC.74.021301

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  • Measurements of the reaction cross sections and momentum distributions for Al-23 neighbouring nuclei Reviewed

    K. Wang, D. Q. Fang, W. Guo, Y. G. Ma, C. W. Ma, T. Z. Yan, X. Z. Cai, W. Q. Shen, Z. Y. Sun, Z. Z. Ren, J. G. Chen, G. H. Liu, E. J. Ma, Y. Shi, Q. M. Su, W. D. Tian, H. W. Wang, C. Zhong, M. Hosoi, T. Izumikawa, R. Kanungo, S. Nakajima, T. Ohnishi, T. Ohtsubo, A. Ozawa, T. Suda, K. Sugawara, T. Suzuki, A. Takisawa, K. Tanaka, T. Yamaguchi, K. Tanaka, T. Yamaguchi, I. Tanihata

    NUCLEAR PHYSICS TRENDS   865   63 - +   2006

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    The reaction cross sections and momentum distributions for Al-23 and its neighbouring nuclei have been measured at the Riken Projectile Fragment Separator (RIPS). The primary beam of 135 A MeV Si-28 was used to produce the secondary beams. The measurement of sigma(R) was carried out by using a transmission-type method. sigma(R) was determined by the ratios between incident and outgoing particles without reaction from both target-in and target-out measurements. P-// of fragment from breakup reactions was determined from the measured TOF between F2 and F3. An enhancement is observed in sigma(R) for Al-23 compared to its neighbors. The P-// of Mg-22 fragments from Al-23 breakup have been obtained. The width of the distributions is found to be consistent with prediction by the Goldhaber Model. The experimental data are discussed in the framework of Glauber model. The analysis of P-// indicates a dominant d-wave component in the ground state of Al-23. This confirms the result of a recent magnetic moment measurement which indicates that the valence proton is in d-wave.

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  • Present and future experiments with stored exotic nuclei at relativistic energies Reviewed

    H. Geissel, Yu. A. Litvinov, B. Pfeiffer, F. Attallah, G. Audi, K. Beckert, P. Beller, F. Bosch, D. Boutin, T. J. Burvenich, L. Chen, T. Faestermann, M. Falch, B. Franzke, M. Hausmann, E. Kaza, T. Kerscher, P. Kienle, O. Klepper, R. Knoebel, C. Kozhuharov, K. -L. Kratz, S. A. Litvinov, K. E. G. Loebner, L. Maier, M. Matos, F. Montes, G. Muenzenberg, C. Nociforo, F. Nolden, Yu. N. Novikov, T. Ohtsubo, A. Ostrowski, Z. Patyk, W. Plass, M. Portillo, T. Radon, H. Schatz, C. Scheidenberger, J. Stadlmann, M. Steck, B. Sun, K. Takahashi, G. Vorobjev, H. Weick, M. Winkler, H. Wollnik, T. Yamaguchi

    FRONTIERS IN NUCLEAR STRUCTURE ASTROPHYSICS, AND REACTIONS: FINUSTAR   831   108 - +   2006

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    Recent progress is presented from experiments on masses and lifetimes of bare and few-electron exotic nuclei at GSI. Relativistic rare isotopes produced via projectile fragmentation and fission were separated in flight by the fragment separator FRS and injected into the storage ring ESR. This worldwide unique experimental technique gives access to all fragments with half-lives down to the microsecond range. The great research potential is also demonstrated by the discovery of new isotopes along with simultaneous measurements of mass and lifetime. Representative results from time-resolved Schottky mass spectrometry are compared with modern theoretical predictions. The measured isospin dependence of pairing-gap energies is not reproduced by conventional mass models. The first direct observation of bound-state beta decay has been achieved. Single particle decay measurements and the continuous recording of both stored mother and daughter nuclei open up a new era for spectroscopy. The combination of stochastic and electron cooling has allowed us to measure with Schottky analysis for the first time short-lived isomers. The future international NUSTAR facility at FAIR consisting of a new large-acceptance in-flight separator (Super-FRS) will be an ideal tool to study the r- and rp-process nuclei.

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  • Nuclear structure study through nuclear moments of mirror pairs Reviewed

    K. Matsuta, T. Nagatomo, A. Ozawa, M. Mihara, R. Matsumiya, K. Yamada, T. Yamaguchi, T. Ohtsubo, S. Momota, T. Izumikawa, T. Sumikama, Y. Nakashima, H. Fujiwara, S. Kumashiro, M. Ota, D. Shinojima, H. Tanaka, T. Yasuno, S. Nakajima, T. Suzuki, K. Yoshida, K. Muranaka, T. Maemura, A. Chiba, Y. Utsuno, M. Fukuda, K. Tanaka, A. Kitagawa, M. Torikoshi, M. Kanazawa, S. Sato, M. Takechi, T. Miyake, M. Ogura, I. Tanihata, Y. Nojiri, K. Minamisono, T. Minamisono, J. R. Alonso, G. F. Krebs

    NUCLEAR PHYSICS TRENDS   865   153 - +   2006

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    beta-NMR spectra have been observed for Cl-33, Al-23 and Ne-23. As a result, the magnetic moment of Cl-33 was determined as vertical bar mu(Cl-33)vertical bar = 0.7549(3) mu(N). Combined with the known magnetic moment of S-33 and the ft-value of the Cl-33 beta decay, the orbital angular momenta and the intrinsic spins for proton and neutron groups, are deduced separately as < l(p)> = 1.3, < I-n > = 0.3, < S-p > = -0.12 and < S-n > = -0.02. The magnetic moment of Al-23, and that of Ne-23 were determined as vertical bar mu(Al-23)vertical bar = 3.89(22) mu(N) and vertical bar mu(Ne-23)vertical bar = 1.0817(9) mu(N), respectively. As a result, the orbital angular momentum < l(z)> and the intrinsic spin < S-z > were deduced to be 2.09(29) and 0.41(29), respectively. Combined with theft-value of the 0 transition from the ground state of Al-23 to the excited state of Mg-23, proton and neutron contributions are separated. The obtained expectation values < l(p)>, < l(n)>, < S-p > and < S-n > are compared with the shell model predictions.

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  • Structure of neutron-rich oxygen isotopes Reviewed

    D Cortina-Gil, J Fernandez-Vazquez, T Aumann, T Baumann, J Benlliure, MJG Borge, LV Chulkov, UD Pramanik, C Forssen, LM Fraile, H Geissel, J Gerl, F Hammache, K Itahashi, R Janik, B Jonson, S Mandal, K Markenroth, M Meister, M Mocko, G Muenzenberg, T Ohtsubo, A Ozawa, Y Prezado, K Riisager, H Scheit, R Schneider, G Schrieder, H Simon, B Sitar, A Stolz, P Strmen, K Suemmerer, Szarka, I, H Weick

    JOURNAL OF PHYSICS G-NUCLEAR AND PARTICLE PHYSICS   31 ( 10 )   S1629 - S1632   2005.10

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    One-nucleon removal reactions at relativistic energies have been used as a spectroscopic tool for obtaining information about the ground state of neutron-rich oxygen isotopes. Using the FRS at GSI, the longitudinal momentum distributions of the emerging fragments after breakup were measured along with the one-nucleon removal cross-sections. The relative contributions of the remaining fragments in their ground and excited states have been determined for a few cases from measurements of gamma rays in coincidence with the longitudinal momentum distribution.. The controversial case of O-23 has been directly addressed. Comparison of our exclusive momentum distributions for the one-neutron removal channel to theoretical momentum distributions calculated with an Eikonal model for the knockout process rendered a spin and parity of I-pi = 1/2(+) for the O-23 ground state. This result resolves the existent experimental discrepancy and supports sub-shell closure at N = 14 with a fairly pure 2s(1/2) neutron in O-23.
    (Some figures in this article are in colour only in the electronic version).

    DOI: 10.1088/0954-3899/31/10/045

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  • Simultaneous measurement of beta(-) decay to bound and continuum electron states Reviewed

    T Ohtsubo, F Bosch, H Geissel, L Maier, C Scheidenberger, F Attallah, K Beckert, P Beller, D Boutin, T Faestermann, B Franczak, B Franzke, M Hausmann, M Hellstrom, E Kaza, P Kienle, O Klepper, HJ Kluge, C Kozhuharov, YA Litvinov, M Matos, G Munzenberg, F Nolden, YN Novikov, M Portillo, T Radon, J Stadlmann, M Steck, T Stohlker, K Summerer, K Takahashi, H Weick, M Winkler, T Yamaguchi

    PHYSICAL REVIEW LETTERS   95 ( 5 )   2005.7

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    We report the first measurement of a ratio lambda(beta b)/lambda(beta c) of bound-state (lambda(beta b)) and continuum-state (lambda(beta c)) beta(-)-decay rates for the case of bare Tl-207(81+) ions. These ions were produced at the GSI fragment separator FRS by projectile fragmentation of a Pb-208 beam. After in-flight separation with the B rho-Delta E-B rho method, they were injected into the experimental storage-ring ESR at an energy of 400.5A MeV, stored, and electron cooled. The number of both the Tl-207(81+) ions and their bound-state beta(-)-decay daughters, hydrogenlike Pb-207(81+) ions, were measured as a function of storage time by recording their Schottky-noise intensities. The experimental result, lambda(beta b)/lambda(beta c)=0.188(18), is in very good agreement with the value of 0.171(1) obtained from theory employing spectra of allowed transitions.

    DOI: 10.1103/PhysRevLett.95.052501

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  • High-rate particle identification of high-energy heavy ions using a tilted electrode gas ionization chamber Reviewed

    K Kimura, T Izumikawa, R Koyama, T Ohnishi, T Ohtsubo, A Ozawa, W Shinozaki, T Suzuki, M Takahashi, Tanihata, I, T Yamaguchi, Y Yamaguchic

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   538 ( 1-3 )   608 - 614   2005.2

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    A high-rate particle identification device for high-energy heavy ions has been developed which utilizes a stacked configuration of grid-less parallel plate gas ionization chambers with thin anode-cathode gaps. The high-rate capability of this chamber was realized by adopting bipolar shaping of anode signals and by the suitable choice of a counter gas. Z-resolutions of 0.2-0.3 were obtained for nuclear fragments of Ar-40 at 95 A MeV with an intensity as high as 10(6) cps. (C) 2004 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nima.2004.08.100

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  • One-neutron knockout of O-23 Reviewed

    D Cortina-Gil, J Fernandez-Vazquez, T Aumann, T Baumann, J Benlliure, MJG Borge, LV Chulkov, UD Pramanik, C Forssen, LM Fraile, H Geissel, J Gerl, F Hammache, K Itahashi, R Janik, B Jonson, S Mandal, K Markenroth, M Meister, M Mocko, G Munzenberg, T Ohtsubo, A Ozawa, Y Prezado, Pribora, V, K Riisager, H Scheit, R Schneider, G Schrieder, H Simon, B Sitar, A Stolz, P Strmen, K Summerer, Szarka, I, H Weick

    EUROPEAN PHYSICAL JOURNAL A   25   343 - 346   2005

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    Breakup reactions were used to study the ground-state configuration of the neutron-rich isotope O-23. The O-22 fragments produced in one-nucleon removal from O-23 at 938 MeV/nucleon in a carbon target were detected in coincidence with de-exciting gamma rays, allowing to discern between 220 ground-state and excited-states contributions. From the comparison of exclusive experimental momentum distributions for the one-neutron removal channel to theoretical momentum distributions calculated in an Eikonal model for the knockout process, and spin and parity assignment of I-pi = 1/2(+) was deduced for the 230 ground state. This result solved the existent experimental discrepancy.

    DOI: 10.1140/epjad/i2005-06-149-2

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  • Magnetic moment of extremely proton-rich nucleus Al-23 Reviewed

    T Nagatomo, K Matsuta, A Ozawa, Y Nakashima, R Matsumiya, M Mihara, T Yasuno, A Chiba, K Yamada, S Momota, T Ohtsubo, M Ohta, D Shinojima, T Izumikawa, H Tanaka, T Yamaguchi, S Nakajima, H Maemura, K Muranaka, S Kumashiro, H Fujiwara, K Yoshida, T Sumikama, K Tanaka, M Ogura, K Minamisono, M Fukuda, T Minamisono, Y Nojiri, T Suzuki, Tanihata, I, Alonso, JR, GF Krebs, TJM Symons

    International Symposium on Correlation Dynamics in Nuclei   20   173 - 174   2005

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    The g-factor of the extremely proton-rich nucleus Al-23 (T-1/2 = 0.47s) has been measured by means of the O-NMR method for the first time. The g-factor were determined as vertical bar g vertical bar = 1.557(88) from the obtained NMR spectra. From the comparison between the experimental value and the shell model calculation, the spin parity of the ground state of Al-23 was determined as I-pi = 5/2(+). Thus, the magnetic moment of Al-23 was determined as vertical bar mu vertical bar = 3.89(22)mu(N).

    DOI: 10.1088/1742-6596/20/1/032

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  • Electric quadrupole momentof Na-25 Reviewed

    K Matsuta, H Fujiwara, T Nagatomo, M Mihara, S Kumashiro, Y Nakashima, M Ogura, S Momota, T Ohtsubo, M Ohta, A Kitagawa, M Kanazawa, M Torikoshi, S Sato, M Fukuda, T Minamisono, Y Nojiri, K Minamisono, M Suda, T Izumikawa, Alonso, JR, GF Krebs, TJM Symons

    International Symposium on Correlation Dynamics in Nuclei   20   169 - 170   2005

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    The electric quadrupole coupling constant eqQ/h of Na-25 (I-pi = 5/2(+), T-1/2 = 59.6 s), implanted in a TiO2 single crystal, has been measured by use of the beta-NMR technique, to determine the electric quadrupole moment Q. As a result, vertical bar eqQ/h vertical bar = (44 +/- 16) kHz and vertical bar Q(Na-25)vertical bar = (1.0 +/- 0.4) mb were determined. From the NMR on 25Na in NaCl, the magnetic moment was determined as vertical bar mu vertical bar = (3.6832 +/- 0.0003) mu(N).

    DOI: 10.1088/1742-6596/20/1/030

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  • Reaction cross-sections for stable nuclei and nucleon density distribution of proton drip-line nucleus B-8 Reviewed

    M Takechi, M Fukuda, M Mihara, T Chinda, T Matsumasa, H Matsubara, Y Nakashima, K Matsuta, T Minamisono, R Koyama, W Shinosaki, M Takahashi, A Takizawa, T Ohtsubo, T Suzuki, T Izumikawa, S Momota, K Tanaka, T Suda, M Sasaki, S Sato, A Kitagawa

    EUROPEAN PHYSICAL JOURNAL A   25   217 - 219   2005

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    The optical limit of the Glauber theory with zero-range approximation, which is successfully used at high energies to connect the nucleon density distribution with reaction cross-sections (sigma(R)), gives somewhat smaller values of sigma(R) by 10-20% at intermediate energies. We have precisely measured the sigma(R) for C-12 on Be, C, and Al at 30A-200A MeV, and for Be-9 on Be at 70A-100A MeV to investigate the enhancement of sigma(R) compared to the optical-limit calculation. From the enhancements, we deduced the nucleon-nucleon range as a function of energies. We deduced the density distribution of B-8 analyzing the known experimental sigma(R) for B-8 with an enhancement correction or with the finite range effect as a test.

    DOI: 10.1140/epjad/i2005-06-078-0

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  • Nuclear structure of light exotic nuclei from break-up reactions Reviewed

    D Cortina, J Fernandez-Vazquez, T Aumann, T Baumann, J Berlliure, MJG Berge, L Chulkov, UD Pramanik, C Forssen, LM Fraile, H Geissel, J Gerl, F Hammache, K Itahashi, R Janik, B Jonson, S Mandal, K Markenroth, M Meister, M Mocko, B Munzenberg, T Ohtsubo, A Ozawa, Y Prezado, Pribora, V, K Riisager, H Scheit, R Schneider, G Schrieder, H Simon, B Sitar, A Stolz, P Strmen, K Summerer, Szarka, I, H Weick

    NUCLEAR PHYSICS A   746   479C - 482C   2004.12

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    One-nucleon removal reactions at relativistic energies have been used as a spectroscopic tool to characterise the ground state properties of several neutron-rich isotopes in the sd-shell. Using the FRS at GSI, the longitudinal momentum distributions of the emerging fragments after one-nucleon removal were measured. The relative contributions of the remaining fragments in their ground and excited states have been determined from measurements of gamma rays in coincidence with the longitudinal momentum distributions. In particular the breakup of O-23 has been investigated. The interpretation of our measurements, in the framework of a simple theoretical model, favours a spin and parity assignment of 1/2(+) for the O-23 ground state in agreement with shell model predictions.

    DOI: 10.1016/j.nuclphysa.2004.09.153

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  • Magnetic moment of Cl-33 Reviewed

    K Matsuta, K Arimura, T Nagatomo, K Akutsu, T Iwakoshi, S Kudo, M Ogura, M Takechi, K Tanaka, T Sumikama, K Minamisono, T Miyake, T Minamisono, M Fukuda, M Mihara, A Kitagawa, M Sasaki, M Kanazawa, M Torikoshi, M Suda, M Hirai, S Momota, Y Nojiri, A Sakamoto, M Saihara, T Ohtsubo, Alonso, JR, GF Krebs, TJM Symons

    NUCLEAR PHYSICS A   746   493C - 496C   2004.12

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    The magnetic moment of Cl-33 (I-pi = 3/2(+), T-1/2 = 2.51 s) has been re-measured precisely by beta-NMR method. The obtained magnetic moment \mu\ = 0.7549(3) mu(N) is consistent with the old value 0.7523(16) mu(N), but is 5 times more accurate. The value is well reproduced by the shell model calculation; mu(SM) = 0.70 mu(N). Combined with the magnetic moment of the mirror partner S-33, the nuclear matrix elements <l(p)>, <l(n)>, <S-p>, and <S-n> were derived.

    DOI: 10.1016/j.nuclphysa.2004.09.075

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  • New results with stored exotic nuclei at relativistic energies Reviewed

    H Geissel, YA Litvinov, F Attallah, K Beckert, P Beller, F Bosch, D Boutin, T Faestermann, M Falch, B Franzke, M Hausmann, M Hellstrom, E Kaza, T Kerscher, O Klepper, HJ Kluge, C Kozhuharov, KL Kratz, SA Litvinov, KEG Lobner, L Maier, M Matos, G Munzenberg, F Nolden, YN Novikov, T Ohtsubo, A Ostrowski, Z Patyk, B Pfeiffer, M Portillo, T Radon, C Scheidenberger, Shishkin, V, J Stadlmann, M Steck, DJ Viera, H Weick, M Winkler, H Wollnik, T Yamaguchi

    NUCLEAR PHYSICS A   746   150C - 155C   2004.12

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    Recently, much progress has been made with stored exotic nuclei at relativistic velocities ((v)/(c) = 0.7). Fragments of Pb-208 and Bi-209 projectiles and fission products from U-238 ions were produced, separated in flight with the fragment separator FRS, and injected into the storage-cooler ring ESR for precision measurements. 114 new masses of neutron-deficient isotopes in the lead region have been measured with time-resolved Schottky Mass Spectrometry (SMS). A new isospin dependence of the pairing energy was observed due to the improved mass accuracy of typically 1.5 x 10(-7) (30 keV). New masses of short-lived neutron-rich fission fragments have been obtained with Isochronous Mass Spectrometry (IMS). An innovative field of spectroscopy has been opened up with lifetime measurements of stored bare and few-electron fragments after applying both stochastic and electron cooling.

    DOI: 10.1016/j.nuclphysa.2004.09.030

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  • Density distribution of B-17 from a reaction cross-section measurement Reviewed

    Y Yamaguchi, C Wu, T Suzuki, A Ozawa, DQ Fang, M Fukuda, N Iwasa, T Izumikawa, H Jeppesen, R Kanungo, R Koyama, T Ohnishi, T Ohtsubo, W Shinozaki, T Suda, M Takahashi, Tanihata, I

    PHYSICAL REVIEW C   70 ( 5 )   2004.11

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    The reaction cross section (sigma(R)) for the neutron-rich nucleus B-17 on a carbon target has been measured at an energy of 77A MeV by the transmission method. An enhancement of sigma(R) at intermediate energy compared to that at high energy was observed. The density distribution of B-17 was deduced through the energy dependence of sigma(R) using a finite-range Glauber-type calculation under an optical-limit approximation as well as a few-body approach. The existence of a long neutron tail in B-17 was demonstrated. The fraction of the wave function with)2)2 the valence two-neutron configuration of (2s(1/2))(J=0)(2) or (1d(5/2))(J=0)(2) was found to be 50+/-10% based on a finite-range few-body Glauber-type calculation.

    DOI: 10.1103/PhysRevC.70.054320

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  • Large hyperfine anomaly between Y-91 and Y-91m in Fe Reviewed

    K Nishimura, S Ohya, T Ohtsubo, Sato, I, J Goto, T Izumikawa, M Tanigaki, A Taniguchi, Y Ohkubo, Y Kawase, S Muto

    PHYSICAL REVIEW B   70 ( 13 )   2004.10

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    Nuclear magnetic resonance on oriented nuclei was carried out using a sample of dilute Y-91 and Y-91m in iron prepared by ion implantation of radioactive precursor Rb isotopes. For (YFe)-Y-91, the beta-ray asymmetry was utilized to measure the magnetic hyperfine interaction frequency, nu(0)=73.566(22) MHz, which led to the magnetic hyperfine field, B-HF=-29.4(2)T, by using the known nuclear g-factor. The field shift of the resonant frequency, dnu(0)/dB(0)=-2.501(17) MHz/T for (YFe)-Y-91, implies a Knight shift value, K=0.0(8)%. The interaction frequency and the field shift of (YFe)-Y-91m obtained via the gamma-ray detection confirmed the previously reported results. A ratio of the measured nu(0) and dnu(0)/dB(0) values for both (YFe)-Y-91 and (YFe)-Y-91m gave rise to the hyperfine anomaly, (91)Delta(91m)=-4.2(8)%, which can explain discrepancies in the B-HF values of YFe as determined by various experiments.

    DOI: 10.1103/PhysRevB.70.132405

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  • Shell structure of the near-dripline nucleus O-23 Reviewed

    D Cortina-Gil, J Fernandez-Vazquez, T Aumann, T Baumann, J Benlliure, MJG Borge, LV Chulkov, UD Pramanik, C Forssen, LM Fraile, H Geissel, J Gerl, F Hammache, K Itahashi, R Janik, B Jonson, S Mandal, K Markenroth, M Meister, M Mocko, G Munzenberg, T Ohtsubo, A Ozawa, Y Prezado, Pribora, V, K Riisager, H Scheit, R Schneider, G Schrieder, H Simon, B Sitar, A Stolz, P Strmen, K Summerer, Szarka, I, H Weick

    PHYSICAL REVIEW LETTERS   93 ( 6 )   2004.8

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    Breakup reactions were used to study the ground-state configuration of the neutron-rich isotope O-23. The O-22 fragments produced in one-nucleon removal from O-23 at 938 MeV/nucleon in a carbon target were detected in coincidence with deexciting gamma rays. The widths of the longitudinal momentum distributions of the O-22 fragments and the one-neutron removal cross sections were interpreted in the framework of a simple theoretical model which favors the assignment of I-pi=1/2(+) to the O-23 ground state.

    DOI: 10.1103/PhysRevLett.93.062501

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  • Study of the density distribution of C-17 from reaction cross section measurement Reviewed

    C Wu, Y Yamaguchi, A Ozawa, R Kanungo, Tanihata, I, T Suzuki, DQ Fang, T Suda, T Ohnishi, M Fukuda, N Iwasa, T Ohtsubo, T Izumikawa, R Koyama, W Shinozaki, M Takahashi

    NUCLEAR PHYSICS A   739 ( 1-2 )   3 - 14   2004.7

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    The reaction cross section of C-17 on a carbon target at 79 A MeV has been measured by the transmission method. The density distribution of C-17 was deduced using the finite-range Glauber model (FRGM) combined with the interaction cross section of C-17 at high energy. The existence of a tail in the density distribution of C-17 is suggested to get a better understanding of both the low energy and high energy data. Under a core plus single-particle assumption, analysis shows a dominant d-wave of the valence neutron in C-17. (C) 2004 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nuclphysa.2004.03.220

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  • Direct mass measurement of bare short-lived V-44, Mn-48, Ti-41 and Cr-45 ions with isochronous mass spectrometry Reviewed

    J Stadlmann, M Hausmann, F Attallah, K Beckert, P Beller, F Bosch, H Eickhoff, M Falch, B Franczak, B Franzke, H Geissel, TH Kerscher, O Klepper, HJ Kluge, C Kozhuharov, YA Litvinov, KEG Lobner, M Matos, G Munzenberg, N Nankov, F Nolden, YN Novikov, T Ohtsubo, T Radon, H Schatz, C Scheidenberger, M Steck, H Weick, H Wollnik

    PHYSICS LETTERS B   586 ( 1-2 )   27 - 33   2004.4

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    We present direct mass measurements of the short-lived V-44, Mn-48, Ti-41 and Cr-45 nuclei. A novel experimental method has been used that is based on projectile fragmentation, in-flight separation of relativistic heavy ions with the fragment separator (FRS). and on isochronous operation of the experimental storage ring (ESR). A mass resolving power of I 10 000 (FWHM) and an accuracy of about (100-500) keV has been achieved. The impact of the present results on the rp-process in X-ray burst models is discussed. (C) 2004 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.physletb.2004.02.014

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  • Precision spectroscopy of pionic 1s states of sn nuclei and evidence for partial restoration of chiral symmetry in the nuclear medium Reviewed

    K Suzuki, M Fujita, H Geissel, H Gilg, A Gillitzer, RS Hayano, S Hirenzaki, K Itahashi, M Iwasaki, P Kienle, M Matos, G Munzenberg, T Ohtsubo, M Sato, M Shindo, T Suzuki, H Weick, M Winkler, T Yamazaki, T Yoneyama

    PHYSICAL REVIEW LETTERS   92 ( 7 )   2004.2

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    Deeply bound 1s states of pi(-) in (115,119,123)Sn were preferentially observed using the Sn(d(3), He) pion-transfer reaction under the recoil-free condition. The 1s binding energies and widths were precisely determined and were used to deduce the isovector parameter of the s-wave pion-nucleus potential to be b(1) = -(0.115+/-0.007)m(pi)(-1). The observed enhancement of \b(1)\ over the free piN value (b(1)(free)/b(1) = 0.78+/-0.05) indicates a reduction of the chiral order parameter, f(pi)*(rho)(2)/f(pi)(2)approximate to0.64, at the normal nuclear density, rho=rho(0).

    DOI: 10.1103/PhysRevLett.92.072302

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  • Halo structure of B-17 studied via its reaction cross section Reviewed

    Y Yamaguchi, T Suzuki, T Ohtsubo, T Izumikawa, W Shinozaki, M Takahashi, R Koyama, S Watanabe, C Wu, A Ozawa, T Ohnishi, DQ Fang, T Suda, R Kanungo, H Jeppesen, Tanihata, I, M Fukuda, N Iwasa

    NEW ERA OF NUCLEAR STRUCTURE PHYSICS   114 - 118   2004

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    The reaction cross section for the neutron-rich nucleus B-17 on a carbon target has been measured at an energy of 77 AMeV by a transmission method. A large enhancement of 17B reaction cross section at low energy was observed. The density distribution of 17B was deduced through the energy dependence of the reaction cross section together with high-energy data using a finite-range Glauber-model calculation under an optical-limit approximation. It is confirmed that the neutron-tail in the density distribution is necessary for 17B in order to reproduce the measured reaction cross sections. Based on the assumption of a core (B-15) plus valence two-neutron picture, the mixture of v(2s(1/2)) and V(1d(5/2)) was studied without treating the correlation between two neutrons.

    DOI: 10.1142/9789812702401_0017

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  • Hyperfine fields of Sr and Y in ferromagnetic hosts, and magnetic moment of Y-93 Reviewed

    K Nishimura, S Ohya, T Ohtsubo, T Izumikawa, M Sasaki, Sato, I, M Suzuji, J Goto, M Tanigaki, A Taniguchi, Y Ohkubo, Y Kawase, S Muto

    HYPERFINE INTERACTIONS   159 ( 1-4 )   239 - 243   2004

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    Recent studies of hyperfine fields B-HF of Sr and Y in Fe are briefly reviewed. The B-HF value of Y in Ni is given by NMRON of (YNi)-Y-91m. The nuclear mangetic moment of the ground state of Y-93 is extracted from the beta-ray detected NMRON of Y-93 Fe.

    DOI: 10.1007/s10751-005-9106-3

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  • Spectroscopy of light exotic nuclei using nuclear break-up Reviewed

    D Cortina-Gil, J Fernandez-Vazquez, T Aumann, T Baumann, J Benlliure, MJG Borge, LV Chulkov, UD Pramanik, C Forssen, LM Fraile, H Geissel, J Gerl, F Hammache, K Itahashi, R Janik, B Jonson, S Mandal, K Markenroth, M Meister, M Mocko, G Munzenberg, T Ohtsubo, A Ozawa, Y Prezado, Pribora, V, K Riisager, H Scheit, R Schneider, G Schrieder, H Simon, B Sitar, A Stolz, P Strmen, K Summerer, Szarka, I, H Weick

    LABYRINTH IN NUCLEAR STRUCTURE   701   112 - 116   2004

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    One-nucleon removal reactions at relativistic energies have been used as spectroscopic tool to obtain information about the ground state properties of several neutron-rich isotopes in the sd-shell. Using the FRS at GSI, the longitudinal momentum distributions of the emerging fragments after one-nucleon removal cross-sections were measured. The relative contributions of the remaining fragments in their ground and excited states have been determined from measurements of gamma rays in coincidence with the longitudinal momentum distributions. The interesting case of O-23 Will be directly address. The interpretation of our experimental results in the framework of a simple theoretical model will favours a spin and parity assignment of 1/2(+) for the O-23 ground state in agreement with shell model predictions.

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  • Study of basic nuclear properties of highly-charged, unstable nuclei at the SIS-FRS-ESR complex Reviewed

    C Scheidenberger, F Attallah, K Beckert, P Beller, F Bosch, D Boutin, H Eickhoff, T Faestermann, M Falch, B Franczak, B Franzke, H Geissel, M Hausmann, M Hellstrom, E Kaza, T Kerscher, O Klepper, HJ Kluge, R Koyama, C Kozhuharov, KL Kratz, YA Litvinov, K Lobner, L Maier, M Matos, G Munzenberg, F Nolden, YN Novikov, T Ohtsubo, A Ostrowski, A Ozawa, Z Patyk, B Pfeiffer, M Portillo, W Quint, T Radon, Shishkin, V, J Stadlmann, M Steck, K Summerer, T Suzuki, MB Trzhaskovskaja, DJ Vieira, S Watanabe, H Weick, M Winkler, H Wollnik, T Yamaguchi

    ACTA PHYSICA HUNGARICA NEW SERIES-HEAVY ION PHYSICS   19 ( 1-2 )   165 - 170   2004

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    Recent progress in experiments with exotic nuclear beams at the SIS-FRS-ESR facility is summarized. New results on gross properties of exotic nuclei like binding energy, half-lives, and decay modes are presented. A brief outlook to future experiments is given.

    DOI: 10.1556/APH.19.2004.1-2.27

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  • Low-temperature nuclear orientation of Pm-144 in metamagnetic (RE)NiAl4 single crystals Reviewed

    K Nishimura, K Mori, S Teraoka, WD Hutchison, DH Chaplin, S Ohya, T Ohtsubo, S Muto, T Shinozuka

    HYPERFINE INTERACTIONS   158 ( 1-4 )   199 - 203   2004

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    Magnetic properties of Pm ions in NdNiAl4 were investigated by low-temperature nuclear orientation of Pm-144. The observed gamma-ray anisotropy as a function of external fields revealed a change in the magnetic structure of Pm ions at the metamagnetic Phase transition of NdNiAl4. The extracted hyperfine field was 50(5) T which is substantially smaller than those previously reported.

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  • Nuclear magnetic resonance on oriented nuclei in (HfFe)-Hf-175 Reviewed

    S Muto, T Ohtsubo, S Ohya, K Nishimura

    HYPERFINE INTERACTIONS   158 ( 1-4 )   195 - 198   2004

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    Nuclear magnetic resonance on oriented Hf-175 in iron host has been measured. Samples of (HfFe)-Hf-175 were made by recoil implantation of the precursor Ta-175 isotope. The resonance frequency and the resonance line width have been determined to be 139.0 (1) MHz and FWHM = 2.7 (2) MHz, respectively, in an external magnetic field of 0.1 T. The resonance width was very narrow compared with the previously reported value of 11.0 (1.1) MHz. With the known value of the magnetic moment of mu(Hf-175) = -0.62 (3) mu(N), the hyperfine field has been deduced as B-HF = -73.6 (3.5) T.

    DOI: 10.1007/s10751-005-9032-4

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  • Magnetic moment of the 3/2(-) ground state of W-185 Reviewed

    T Ohtsubo, S Ohya, S Muto

    HYPERFINE INTERACTIONS   159 ( 1-4 )   277 - 280   2004

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    Nuclear magnetic resonance measurement have been performed for W-185 oriented at 8 mK in in Fe host. The magnetic hyperfine splitting frequency at ail external magnetic field of 0.1 T was determined to be 196.6(2) MHz. With the known hyperfine field of B-hf=71.4(18) T, the nuclear magnetic moment of W-185 is deduced as mu(W-185)=+0.543(14) mu(N).

    DOI: 10.1007/s10751-005-9111-6

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  • Quadrupole moments of Na isotopes Reviewed

    M Ogura, T Nagatomo, K Minamisomo, K Matsuta, T Minamisono, Y Nakashima, CDP Levy, T Sumikama, M Mihara, H Fujiwara, S Kumashiro, M Fukuda, JA Behr, KP Jackson, S Momota, Y Nojiri, T Ohtsubo, M Ohta, A Kitagawa, M Kanazawa, M Torikoshi, S Sato, M Suda, Alonso, JR, GF Krebs, TM Symons

    HYPERFINE INTERACTIONS   159 ( 1-4 )   235 - 238   2004

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    The electric quadrupole coupling constants eqQ/h of Na-20 (I-pi=2(+), t(1/2)=449.7 ms) Na-21(I-pi=3/2, T-1/2=22.49 s) and Na-25 (I-pi=5/2, T-1/2=59.6 s) in single crystal ZnO and TiO2 were precisely measured by applying the beta-NMR technique. The ratio of the quadrupole moments between Na-20 (Na-25) and Na-21 was determined to be 0.728 +/- 0.023 (0.011 +/- 0.002).

    DOI: 10.1007/s10751-005-9105-4

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  • Magnetic moment and spin of the extremely proton-rich nucleus Al-23 Reviewed

    K Matsuta, Y Nakashima, T Nagatomo, A Ozawa, K Yamada, M Mihara, S Kumashiro, H Fujiwara, S Momota, M Ota, T Ohtsubo, K Yoshida, T Sumikama, M Ogura, K Minamisono, M Fukuda, T Minamisono, Y Nojiri, T Suzuki, T Izumikawa, Tanihata, I, Alonso, JR, GF Krebs, TJM Symons

    HYPERFINE INTERACTIONS   159 ( 1-4 )   257 - 260   2004

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    The g-factor of the exteremely proton-rich Al-23(T-1/2=0.47 s) has been measured for the first time, applying beta-NMR technique on this nucleus implanted in Si. The obtained vertical bar g vertical bar=(1.58 +/- 0.2) suggests that the spin of the ground state of Al-23 is 5/2. The magnetic moment is determined as vertical bar mu vertical bar = (3.95 +/- 0.55) mu(N).

    DOI: 10.1007/s10751-005-9115-2

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  • Magnetic hyperfine anomaly measurements using nuclear magnetic resonance on oriented nuclei Reviewed

    T Ohtsubo, S Ohya, M Sasaki, T Izumikawa, K Nishimura, J Goto, M Tanigaki, A Taniguchi, Y Ohkubo, Y Kawase, S Muto

    NEW ERA OF NUCLEAR STRUCTURE PHYSICS   297 - 301   2004

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    Nuclear magnetic resonance on oriented nuclei for (YFe)-Y-91 experiments have been performed. Comparing the external field dependence of resonance frequencies with (YFe)-Y-91 and (YFe)-Y-91m, the hyperfine anomaly in Fe was determined as (91m)Delta(91) = +4.2(8)%. The measured hyperfine anomaly was interpreted in terms of a microscopic theory including core polarization and meson exchange currents.

    DOI: 10.1142/9789812702401_0045

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  • Measurements of the interaction cross sections for Ar and Cl isotopes (vol 709, pg 60, 2002) Reviewed

    A Ozawa, T Baumann, L Chulkov, D Cortina, U Datta, J Fernandez, H Geissel, F Hammache, K Itahashi, M Ivanov, R Janik, T Kato, K Kimura, T Kobayashi, K Markenroth, M Meister, G Munzenberg, T Ohtsubo, S Ohya, T Okuda, AA Ogloblin, Pribora, V, M Sekiguchi, B Sitar, P Strmen, S Sugimoto, K Summerer, T Suzuki, Tanihata, I, Y Yamaguchi

    NUCLEAR PHYSICS A   727 ( 3-4 )   465 - 466   2003.11

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    DOI: 10.1016/j.nuclphysa.2003.08.020

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  • Nuclear magnetic resonance on oriented nuclei of (SrFe)-Sr-91 Reviewed

    K Nishimura, S Ohya, T Ohtsubo, M Sasaki, J Goto, T Izumikawa, M Tanigaki, A Taniguchi, Y Ohkubo, Y Kawase, S Muto

    PHYSICAL REVIEW B   68 ( 1 )   2003.7

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    Nuclear magnetic resonance on oriented nuclei was used in combination with beta-ray detection and ion implantation, leading to the successful observation of the resonance of (SrFe)-Sr-91. The magnetic hyperfine field (B-HF) was deduced as B-HF(SrFe)=-23.83(7) T using the known nuclear g factor. This result explains the existing problem of disagreement in B-HF values for SrFe between theory and experiment. An experimental nuclear spin-lattice relaxation rate was obtained and is briefly discussed in comparison with a theoretical estimate.

    DOI: 10.1103/PhysRevB.68.012403

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  • NMR-ON studies on the magnetic hyperfine field at La-140 in Fe Reviewed

    J Goto, M Tanigaki, AI Taniguchi, Y Ohkubo, Y Kawase, S Ohya, K Nishimura, T Ohtsubo, S Muto

    JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN   72 ( 3 )   723 - 726   2003.3

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    Nuclear magnetic resonance on oriented nuclei (NMR-ON) of La existing as a dilute impurity in Fe was observed for the first time. NMR-ON experiments were performed by detecting the 1596 keV gamma rays from the beta decay of La-140 in external magnetic fields of 0.1, 0.1 0.4 and 0.6 T. From the external magnetic-field dependence of the resonance frequency. the magnetic hyperfine field and the Knight shift were deduced to be B-hf = -47 +/- 1 T and K = -4.0 +/- 3.4% respectively. The effective relaxation time of (LaFe)-La-140 at 8 mK in an external magnetic field of 0.2 T was determined to be 8.8 +/- 1.5 min using a single-exponential fit. The present value of the magnetic hyperfine field agrees with that deduced from a two-site model by the low-temperature nuclear orientation method.

    DOI: 10.1143/JPSJ.72.723

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  • New results on B-8 and O-23 ground state properties Reviewed

    D Cortina-Gil, J Fernandez-Vazquez, F Attallah, T Baumann, J Benlliure, MJG Borge, L Chulkov, C Forssen, LM Fraile, H Geissel, J Gerl, K Ithashi, R Janik, B Jonson, S Karlsson, H Lenske, S Mandal, K Markenroth, M Meister, M Mocko, G Munzenberg, T Ohtsubo, A Ozawa, Y Parfenova, Pribora, V, A Richter, K Riisager, R Schneider, H Scheit, G Schrieder, N Shulgina, H Simon, B Sitar, A Stolz, P Strmen, K Summerer, Szarka, I, S Wan, H Weick, M Zhukov

    FRONTIERS OF NUCLEAR STRUCTURE   656   315 - 322   2003

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    One-nucleon removal reactions at relativistic energies have been used as spectroscopic tool to obtain information about the ground state properties of B-8 and O-23. Using the FRS at GSI, the longitudinal momentum distributions of the emerging fragments after breakup and the one-nucleon removal cross-sections were measured. The relative contributions of the remaining fragments (Be-7 and O-22) in their ground and excited states have been determined from measurements of gamma rays in coincidence with the longitudinal momentum distributions. In the B-8 case, the experimental breakup data on two different targets (C and Pb) allow a determination of the weight of the Be-7* component in the B-8 ground state wave function as (13.3+/-2.2) %. These results are discussed in the context of a theoretical three-body model. Preliminary results on O-23 indicate a spin and parity assignment of 1/2(+) in agreement with shell model predictions.

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  • Observation of pionic 1s states in Sn nuclei and its implications on chiral symmetry restoration Reviewed

    K Suzuki, M Fujita, H Geissel, H Gilg, A Gillitzer, RS Hayano, S Hirenzaki, K Itahashi, M Iwasaki, P Kienle, M Matos, G Munzenberg, T Ohtsubo, M Sato, M Shindo, T Suzuki, H Weick, M Winkler, T Yamazaki, T Yoneyama

    PROGRESS OF THEORETICAL PHYSICS SUPPLEMENT   ( 149 )   32 - 41   2003

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    We observed deeply bound pi(-) Is states in Sn-115,Sn-119,Sn-123 for the first time in (116,120,124) Sn(d, He-3) reactions at recoil free conditions to determine the 1s binding energies and the widths precisely. A preliminary result is used to deduce the isovector scattering amplitude as b(1) = 0.115 +/- 0.005 m(pi)(-1). The observed enhancement of b(1) over the free piN value infers 35% reduction of f(pi)(2) at the normal nuclear density, rho = 0.17 fm(-3).

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  • Recent studies on the nuclear moments of light mirror nuclei (T = 1/2, 3/2) Reviewed

    K Matsuta, T Minamisono, M Fukuda, M Mihara, K Sato, K Minamisono, T Yamaguchi, T Onishi, Miyake, I, M Sasaki, M Tanigaki, T Ohtsubo, S Momota, Y Nojiri, K Yoshida, A Ozawa, Tanihata, I, A Kitagawa, M Torikoshi, M Kanazawa, S Koda, T Nishio, M Suda, Alonso, JR, GF Krebs, TJM Symons, SS Hanna

    NUCLEAR PHYSICS A   704   98C - 106C   2002.6

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    Nuclear moments of several unstable nuclei with isospin T = 1/2 and 3/2, including exotic ones have been determined by the beta-NMR technique together with the polarized radioactive nuclear beams technique by the Osaka-RIKEN-HIMAC-LBL Collaboration. The results and their implications with respect to the nuclear structure of the unstable nuclei are discussed.

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  • Precise magnetic moment of short-lived beta emitter Ar-35 Reviewed

    K Matsuta, T Tsubota, C Ha, T Miyake, M Sasaki, K Sato, K Minamisono, K Tanaka, S Kaminaka, A Takemura, T Sumikama, T Nagatomo, K Hashimoto, M Mihara, M Fukuda, T Minamisono, T Ohtsubo, Y Nojiri, S Momota, A Kitagawa, M Torikoshi, M Kanazawa, S Koda, T Nishio, M Suda, J Alonso, GF Krebs, TJM Symons

    NUCLEAR PHYSICS A   701   383C - 386C   2002.4

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    The magnetic moment of the short-lived beta emitter Ar-35 (I-pi = 3/2(+), T-1/2 = 1.77 s) has been remeasured by means of the combined technique of polarized nuclear beams and beta-NMR. The obtained magnetic moment is 0.6322(2) mu(N). This value is consistent with the old data, but is one order of more magnitude precise. The value is well reproduced by the shell model calculation. (C) 2002 Elsevier Science B.V. All rights reserved.

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  • Nuclear magnetic moment of the Ce-143 ground state Reviewed

    A Taniguchi, Y Kawase, Y Ohkubo, J Goto, T Ohtsubo, S Ohya

    PHYSICAL REVIEW C   65 ( 1 )   2002.1

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    The nuclear magnetic moment of the Ce-143 ground state (T-1/2 = 33.0 h, I-pi = 3/2(-)) has been measured with the technique of nuclear magnetic resonance on oriented nuclei (NMR-ON) at low temperature. A sample ((CeFe)-Ce-143) was prepared by implanting into an Fe foil nuclei of mass number 143, which were separated from fission products with an on-line isotope separator. The NMR-ON spectra were obtained by detecting specific beta and gamma rays, and the resonance frequency was thereby determined to be 84.3(1) MHz. Using the reported value of the hyperfine magnetic field at other Ce nuclei in Fe, the nuclear magnetic moment of the Ce-143 ground state was determined to be \mu\ = 0.43(1) mu(N). This value is discussed based on a systematics of the magnetic moments of other N = 85 nuclei.

    DOI: 10.1003/PhysRevC.65.017301

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  • Direct observation of bound state beta decay of bare Tl-207 at FRS-ESR Reviewed

    T Ohtsubo, F Bosch, H Geissel, C Scheidenberger, F Attallah, K Beckert, P Beller, T Fastermann, B Franzke, M Hausmann, M Hellstrom, P Kienle, O Klepper, C Kozhuharov, Y Livitnov, L Maier, G Munzenberg, F Nolden, Y Novikov, T Radon, Shishkin, V, J Stadlmann, M Steck, T Stohlker, K Summer, H Weick, M Winkler

    PROGRESS OF THEORETICAL PHYSICS SUPPLEMENT   ( 146 )   493 - 497   2002

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    We observed the bound-state beta decay of fully ionized Tl-207 nuclei circulating in a storage ring. It is the first direct measurement of bound-state beta decay. Tl-207 nuclei were produced by the projectile fragmentation, separated by fragment separator and injected in the storage ring. Using the Schottky diagnostics the decay time spectrum of bare Tl-207 and hydrogen like Pb-207 ions which are the,daughter nuclei of bound-state beta decay were measured. Observed decay-rate ratio between bound-state and continuous-state beta decay was 0.18(2). This value is consistent with the theoretical calculation.

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  • Development of a gas-catcher system to stop relativistic ions at GSI. Reviewed

    G Savard, C Scheidenberger, P Dendooven, P Van Duppen, S Elisseev, T Faestermann, H Geissel, M Hausmann, M Hellstroem, CL Jiang, E Kaza, B Kindler, Y Litvinov, B Lommel, M Maier, D Morrissey, C Muenzenberg, JA Nolen, T Ohtsubo, B Sherrill, Shishkin, V, GD Sprouse, K Suemmerer, Tanihata, I, M Wada, H Weick, M Weidenmueller, BJ Zabransky

    ABSTRACTS OF PAPERS OF THE AMERICAN CHEMICAL SOCIETY   222   U15 - U15   2001.8

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  • Progress in mass measurements of stored exotic nuclei at relativistic energies Reviewed

    H Geissel, F Attallah, K Beckert, F Bosch, M Falch, B Franzke, M Hausmann, T Kerscher, O Klepper, HJ Kluge, C Kozhuharov, Y Litvinov, KEG Lobner, G Munzenberg, N Nankov, F Nolden, Y Novikov, T Ohtsubo, Z Patyk, T Radon, C Scheidenberger, J Stadlmann, M Steck, K Summerer, H Weick, H Wollnik

    NUCLEAR PHYSICS A   685   115C - 126C   2001.3

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    Exotic nuclei produced via projectile fragmentation were separated in flight by the fragment separator FRS and injected into the storage ring ESR at (300-400) MeV/u. Ultra-cold fragment beams with half-lives larger than 10 s were investigated by Schottky Mass Spectroscopy (SMS) applying electron cooling. A new efficient data acquisition system recorded the time correlations allowing corrections for possible drifts of the revolution frequencies. In addition, it allows to observe the nuclear decay of the fragments circulating in the ESR. Representative results of previously unknown masses of about 150 neutron-deficient isotopes in the range of 52 less than or equal to Z less than or equal to 85 are discussed. Results for lead isotopes are compared with different mass models. Exotic nuclei with half-lives shorter than the time required for electron cooling have been investigated by time-of-flight measurements with the ESR being operated in the isochronous mode. This novel experimental technique gives access to all nuclei with half-lives down to the microsecond range and has been successfully applied in first experiments with light fragments produced by Cr-52 and Kr-84 projectiles. A mass resolving power of better than m/Deltam = 0.9 . 10(5) (FWHM) was achieved with isochronous mass spectrometry (IMS).

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  • Magnetic hyperfine fields of Pm-151(Fe)under-bar and Nd-147(Ni)under-bar Reviewed

    J Goto, S Ohya, T Ohtsubo, Y Kawamura, S Muto, K Nishimura, M Tanigaki, A Taniguchi, Y Ohkubo, Y Kawase

    HYPERFINE INTERACTIONS   136   561 - 566   2001

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    Low-temperature nuclear orientation (LTNO) experiments were performed on Pm-151 implanted into iron and Nd-147 implanted into nickel. The gamma-ray anisotropy measurements yielded values of the magnetic hyperfine field and the substitutional fractions of these ions in the host metals. An observed discrepancy between the substitutional fractions obtained from the 91 keV and 531 keV data on Nd-147 (Ni) under bar is briefly discussed.

    DOI: 10.1023/A:1020583010083

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  • Knight shift of Nb-90, Mo-93m, Tc-96, and Rh-101m in Nb using brute-force NMRON Reviewed

    K Nishimura, S Ohya, Y Kawamura, T Ohtsubo, T Izumikawa, S Muto

    HYPERFINE INTERACTIONS   136   567 - 572   2001

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    Brute-force nuclear magnetic resonance on oriented nuclei (BF-NMRON) of Nb-90, Mo-93m, Tc-96, and Rh-101m was carried out in a new host metal, Nb. The resonance center frequencies at an external field of 11.922(6) T were obtained as v((NbNb)-Nb-90) = 56.572(9) MHz, v((MoNb)-Mo-93m) = 85.76(3) MHz, v((TcNb)-Tc-96) = 66.997(11) MHz, and v(Rh-101m Nb) = 111.010(19) MHz. A systematic analysis of the Knight shift of 4d elements in extremely dilute alloy systems is briefly discussed.

    DOI: 10.1023/A:1020535110992

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  • Isochronous mass measurements of hot exotic nuclei Reviewed

    M Hausmann, J Stadlmann, F Attallah, K Beckert, P Beller, F Bosch, H Eickhoff, M Falch, B Franczak, B Franzke, H Geissel, T Kerscher, O Klepper, HJ Kluge, C Kozhuharov, YA Litvinov, KEG Lobner, G Munzenberg, N Nankov, F Nolden, YN Novikov, T Ohtsubo, T Radon, H Schatz, C Scheidenberger, M Steck, Z Sun, H Weick, H Wollnik

    HYPERFINE INTERACTIONS   132 ( 1-4 )   291 - 297   2001

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    A novel method for mass measurements of short-lived exotic nuclides is presented. Exotic nuclides were produced and separated in flight at relativistic energies: with the fragment separator (FRS) and were injected into the experimental storage ring (ESR). Operating the ESR in the isochronous mode we performed mass measurements of neutron deficient fragments of Kr-84 with half-lives larger than 50 ms. However, this experimental technique is applicable in a half-life range down to a few mus. A mass resolving power of 110000 (FWHM) has been achieved. Results are presented for the masses of As-68, Se-70,Se-71 and Br-73.

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  • One-nucleon removal reactions at the FRS Reviewed

    D Cortina-Gil, F Attallah, T Aumann, L Axelsson, T Baumann, J Benlliure, MJG Borge, K Boretzky, L Chulkov, UD Pramanik, J Fernandez, L Fraile, H Geissel, J Gerl, F Hammache, Hansper, V, K Itahashi, M Ivanov, R Janik, B Jonson, H Lenske, S Mandal, K Markenroth, M Meister, M Mocko, G Munzenberg, T Ohtsubo, A Ozawa, Y Prezado, Pribora, V, K Riisager, B Sitar, P Strmen, Szarka, I, C Scheidenberger, K Schmidt, G Schrieder, K Summerer, T Suzuki, H Weick

    ACTA PHYSICA HUNGARICA NEW SERIES-HEAVY ION PHYSICS   12 ( 2-4 )   275 - 279   2000

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    The fragment separator FRS at GSI was used as an energy-loss spectrometer to study the nuclear structure of exotic light nuclei via nucleon-removal reactions. The measurements performed include the longitudinal momentum distributions of fragments after one-nucleon removal, the one-nucleon removal cross-sections and in some cases the coincident detection of gamma rays emitted from the breakup fragments. The isotopes studied range from 5 < Z < 8.

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  • Density distribution of B-8 studied via reaction cross sections Reviewed

    M Fukuda, M Mihara, T Fukao, S Fukuda, M Ishihara, S Ito, T Kobayashi, K Matsuta, T Minamisono, S Momota, T Nakamura, Y Nojiri, Y Ogawa, T Ohtsubo, T Onishi, A Ozawa, T Suzuki, M Tanigaki, Tanihata, I, K Yoshida

    NUCLEAR PHYSICS A   656 ( 2 )   209 - 228   1999.8

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    Reaction cross sections (sigma(R)) for B-8 on Be, C and Al targets were measured at energies of 40A and 60A MeV. The density distribution of B-8 was Studied through a chi(2)-fitting procedure on the sigma(R) including the high-energy data using the optical limit of Glauber theory with assumptions on the enhancement of the sigma(R) at low energies. The result shows a long tail in the density distribution. Large one-proton removal cross sections were also observed to support the existence of a long proton tail consistent with its binding energy. (C) 1999 Elsevier Science B.V. All rights reserved.

    DOI: 10.1016/S0375-9474(99)00308-5

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  • Quadrupole moments of short-lived beta-emitters O-13,O-19 and F-21 Reviewed

    K. Sato, M. Tanigaki, T. Onishi, M. Fukuda, T. Minamisono, M. Mihara, K. Matsuta, S. Takeda, M. Sasaki, T. Yamaguchi, T. Miyake, K. Minamisono, A. Morishita, F. Osumi, Y. Muramoto, S. Oui, T. Fukao, Y. Matsumoto, T. Ohtsubo, S. Fukuda, Y. Nojiri, S. Momota, K. Yoshida, A. Ozawa, T. Kobayashi, I. Tanihata, A. Kitagawa, M. Torikoshi, H. Sagawa, H. Kitagawa, G. F. Krebs, J. R. Alonso, T. J. M. Symons

    NUCLEAR PHYSICS A   654 ( 1 )   735C - 738C   1999.7

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    The quadrupole moments of the short-lived, beta-emitting nuclei O-13 (I-pi = 3/2(-), T-1/2 = 8.6 ms), O-19 (I-pi = 5/2(+), T-1/2 = 27 s) and F-21 (I-pi = 5/2(+), T-1/2 = 4.3 s) were determined to be |Q(O-13)| = 11.0 +/- 1.3 mb, |Q(O-19)| = 3.7 +/- 0.4 mb and |Q(F-21)| = 110 +/- 22 mb by detecting their beta-NMR. The present results are compared with the theoretical values obtained by the Hartree Fock calculations taking their one nucleon-separation energies into account.

    DOI: 10.1016/S0375-9474(00)88538-3

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  • Electromagnetic moments of short lived beta emitters F-21, Mg-23, Si-27 and Ca-39 Reviewed

    K Matsuta, T Onishi, M Fukuda, T Minamisono, H Akai, M Sasaki, T Yamaguchi, T Miyake, K Sato, K Minamisono, F Ohsumi, Y Muramoto, S Oui, C Ha, K Tanaka, K Kidera, A Morishita, A Kitagawa, M Torikoshi, M Kanazawa, T Nishio, S Koda, T Ohtsubo, S Fukuda, Y Nojiri, S Momota, A Ozawa, K Yoshida, T Suzuki, T Kobayashi, Tanihata, I, SS Hanna, Alonso, JR, GF Krebs, TJM Symons

    HYPERFINE INTERACTIONS   120 ( 1-8 )   673 - 677   1999

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    The beta-NMR spectra of F-21, Mg-23, Si-27 and Ca-39 which were produced in heavy ion collisions and implanted in various crystals have been observed. The magnetic moments of F-21 and Si-27 were determined to be \mu(F-21)\ = 3.9194 +/- 0.0012 mu(N) and \mu(Si-27)\ = 0.8653 +/- 0.0003 mu(N), respectively. The electric quadrupole coupling constants were determined for the first time to be \eqQ(F-21 in MgF2)/h\ = 9.94 +/- 0.09 MHz, \eqQ(Mg-23 in MgF2)/h\ = 1.96 +/- 0.06 MHz, \eqQ(Si-27 in Al2O3)/h\ = 1.90 +/- 0.12 MHz, \eqQ(Ca-39 in CaCO3)/h\ = 0.60 +/- 0.04 MHz. From the present eqQ/h, the Q moments were deduced as \Q(F-21)\ = 110 +/- 22 mb, \Q(Mg-23)\ = 114 +/- 3 mb, \Q(Si-27)\ = 60 +/- 13 mb and \Q(Ca-39)\ = 36 +/- 7 mb. The present data were compared with the theoretical values obtained by the OXBASH shell model code.

    DOI: 10.1023/A:1017036009679

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  • Spin polarization of beta-emitting fragments in high energy heavy ions on Be collisions Reviewed

    K Matsuta, T Onishi, M Fukuda, T Minamisono, M Mihara, M Sasaki, T Yamaguchi, T Miyake, K Sato, K Minamisono, F Ohsumi, Y Muramoto, S Oui, C Ha, K Tanaka, K Kidera, A Morishita, T Tsubota, T Sumikama, A Kitagawa, M Torikoshi, M Kanazawa, T Nishio, S Koda, T Ohtsubo, S Fukuda, Y Nojiri, S Momota, A Ozawa, K Yoshida, T Suzuki, T Kobayashi, Tanihata, I, SS Hanna, Alonso, JR, GF Krebs, TJM Symons

    HYPERFINE INTERACTIONS   120 ( 1-8 )   713 - 717   1999

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    The degrees of nuclear spin polarization of B-8,B-12, C-9, N-12, O-13, F-20,F-21, Mg-23, Si-27 and Ca-39 produced in the high energy C-12,C-13, O-16, Ne-22, Mg-24, Si-28 and Ca-40 ions on Be collisions have been measured systematically, for the technical developments of the nuclear moment studies as well as the hyperfine interaction studies by means of beta-NMR technique. The fragment momentum dependences were well reproduced by the simple kinematical model. Incident energy dependence and the mass dependence as well as the reaction angle dependences were qualitatively explained by the mixing of the near and far side collisions.

    DOI: 10.1023/A:1017000429243

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  • Knight shifts for short-lived beta emitters in Pt Reviewed

    K Matsuta, T Minamisono, M Tanigaki, T Onishi, M Fukuda, M Mihara, H Akai, M Sasaki, T Yamaguchi, T Miyake, K Sato, K Minamisono, C Ha, K Tanaka, K Kidera, A Morishita, S Kaminaka, T Tsubota, T Sumikama, A Kitagawa, M Torikoshi, M Kanazawa, T Nishio, S Koda, T Ohtsubo, Y Nojiri, S Momota, SS Hanna, Alonso, JR, GF Krebs, TJM Symons

    HYPERFINE INTERACTIONS   120 ( 1-8 )   719 - 723   1999

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    The Knight shifts K for short-lived beta emitters N-12 and Si-27 implanted in Pt have been measured by means of beta-NMR technique. The results were K(N-12 in Pt) = +(5.8 +/- 2.1) X 10(-4) and K(Si-27 in Pt) = +(1.4 +/- 0.8) X 10(-3). The spin-lattice relaxation time T-1 was measured for N-12 in Pt. The result was T-1(N-12 in Pt, T = 300 K) = 66 +/- 8 ms, thus, T1T = 20 +/- 2 Ks. The present Knight shifts are in good agreement with the KKR band structure calculation with local lattice relaxation determined theoretically.

    DOI: 10.1023/A:1017052413313

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  • Hyperfine interactions of O-19 in TiO2 and quadrupole moments of O-13,O-19 Reviewed

    K Sato, T Miyake, A Morishita, K Matsuta, T Minamisono, M Tanigaki, S Takeda, M Mihara, M Fukuda, Y Nojiri, K Minamisono, T Fukao, Y Matsumoto, T Ohtsubo, S Fukuda, S Momota, K Yoshida, A Ozawa, T Kobayashi, Tanihata, I, H Sagawa, H Kitagawa, GF Krebs, Alonso, JR, TJM Symons

    HYPERFINE INTERACTIONS   120 ( 1-8 )   661 - 665   1999

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    The electric quadrupole interaction of O-19(I-pi = (5/2)(+), T-1/2 = 27.0 s) in TiO2 single crystal was studied in detail by means of the beta-NQR to determine the electric quadrupole moments Q of short-lived beta-emitting nuclei O-19 and O-13(I-pi = (3/2)(-) T-1/2 = 8.6 ms). Two implantation sites were found for the implanted O nucleus and the quadrupole coupling constants of O-19 at these sites were determined. We observed FT-NMR of the enriched stable isotope O-17 in TiO2 and obtained the electric field gradient (EFG) at the oxygen substitutional site. With this knowledge, we have determined Q(O-13) = 11.0 +/- 1.3 mb and Q(O-19) = 3.7 +/- 0.4 mb. The present results are compared with the theoretical values calculated by the shell model code, OXBASH and by the Hartree-Fock calculation with the realistic potential.

    DOI: 10.1023/A:1017031908770

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  • Magnetic hyperfine interaction of Br in Ni Reviewed

    S Muto, T Ohtsubo, K Yamaguchi, S Ohya

    HYPERFINE INTERACTIONS   120 ( 1-8 )   221 - 224   1999

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    Language:English   Publishing type:Research paper (scientific journal)   Publisher:SPRINGER  

    The magnetic hyperfine splitting frequency of (BrNi)-Br-82 in an external magnetic field of 0.2 T has been measured by NMR-ON method at 8 mK. The centre of resonance frequency was determined to be 18.7(2) MHz. With the known g-factor of g(Br-82) = 0.3254(1), the hyperfine field of (BrNi)-Br-82 was deduced as B-hf((BrNi)-Br-82) = 7.34(8) T. The measured value is compared with the calculated value based on band structure using bonding states.

    DOI: 10.1023/A:1017067105194

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  • Hyperfine interaction of O-13 and Mg-23 implanted in Pt Reviewed

    K Matsuta, M Fukuda, M Tanigaki, T Minamisono, Y Nojiri, H Akai, T Izumikawa, M Nakazato, M Mihara, T Yamaguchi, A Harada, M Sasaki, T Miyake, T Onishi, K Minamisono, T Fukao, K Sato, Y Matsumoto, T Ohtsubo, S Fukuda, K Yoshida, A Ozawa, S Momota, T Kobayashi, Tanihata, I, Alonso, JR, GF Krebs, TJM Symons

    HYPERFINE INTERACTIONS   97-8 ( 1-4 )   501 - 508   1996

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    The spin relaxation time T-1 for short-lived beta emitters O-13 and Mg-23 implanted in Pt have been measured for the first time; T1T(O-13) = 2.90 +/- 0.65 Ks and T1T( Mg) = 1665 +/- 140 Ks. The Knight shift for O-13 in Pt was measured at 300 K to be K(O-13) = +(4.23 +/- 0.14) x 10(-3). In the case of O-13, the Knight shift is unusually large and the relaxation time is unusually fast compared with other interstitial impurities in Pt. A KKR band-structure calculation reproduces the present large Knight shift fairly well.

    DOI: 10.1007/BF02150192

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  • Magnetic moments of proton drip-line nuclei O-13 and C-9 Reviewed

    K Matsuta, T Minamisono, M Tanigaki, M Fukuda, Y Nojiri, M Mihara, T Onishi, T Yamaguchi, A Harada, M Sasaki, T Miyake, K Minamisono, T Fukao, K Sato, Y Matsumoto, T Ohtsubo, S Fukuda, S Momota, K Yoshida, A Ozawa, T Kobayashi, Tanihata, I, Alonso, JR, GF Krebs, TJM Symons

    HYPERFINE INTERACTIONS   97-8 ( 1-4 )   519 - 526   1996

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    The magnetic moments of the proton drip-line nuclei O-13(I-pi = 3/2(-), T-1/2 = 8.6 ms) and C-9(I-pi = 3/2(-), T-1/2 126 ms) have been determined for the first time through the combined techniques of polarized radioactive nuclear beams and beta-NMR detection. The observed magnetic moments are \mu(O-13)\ = 1.3891 +/- 0.0003 mu(N) and \mu(C-9)\ = 1.3914 +/- 0.0005 mu(N). Spin expectation values (sigma) are deduced to be 0.76 and 1.44 for O-13 and C-9, respectively. While the (sigma) of O-13 is consistent with the systematics from isospin T = 1/2 mirror pairs, the (sigma) of C-9 is unusually large, even far larger than the single particle value, (sigma) = 1.

    DOI: 10.1007/BF02150194

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  • Spin polarization of Mg-23 in Mg-24+Au, Cu and Al collisions at 91 A MeV Reviewed

    K MATSUTA, S FUKUDA, T IZUMIKAWA, M TANIGAKI, M FUKUDA, M NAKAZATO, M MIHARA, T ONISHI, T YAMAGUCHI, T MIYAKE, M SASAKI, A HARADA, T OHTSUBO, Y NOJIRI, T MINAMISONO, K YOSHIDA, A OZAWA, T KOBAYASHI, TANIHATA, I, ALONSO, JR, GF KREBS, TJM SYMONS

    POLARIZATION PHENOMENA IN NUCLEAR PHYSICS   ( 339 )   623 - 628   1995

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  • Recent magnetic-moment measurements with polarized radioactive beams Reviewed

    K Matsuta, M Tanigaki, M Fukuda, T Minamisono, Y Nojiri, M Mihara, T Ohnishi, T Yamaguchi, A Harada, M Sasaki, T Miyake, K Minamisono, T Fukao, K Sato, Y Matsumoto, T Ohtsubo, S Fukuda, S Momota, K Yoshida, A Ozawa, T Kobayashi, Tanihata, I, Alonso, JR, GF Krebs, TJM Symons

    ENAM 95 - INTERNATIONAL CONFERENCE ON EXOTIC NUCLEI AND ATOMIC MASSES   43 - 52   1995

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  • PRODUCTION OF UNSTABLE NUCLEI FAR FROM THE STABILITY LINE - ITS SCOPE AND LIMITATIONS Reviewed

    K MATSUTA, A OZAWA, Y NOJIRI, T MINAMISONO, M FUKUDA, S MOMOTA, T OHTSUBO, S FUKUDA, K SUGIMOTO, TANIHATA, I, K YOSHIDA, K OMATA, ALONSO, JR, GF KREBS, TJM SYMONS

    HYPERFINE INTERACTIONS   80 ( 1-4 )   1219 - 1238   1993

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    Recent improvements in isotope separators can be utilized along with the availability of a wide range of nuclear species from the heavy-ion fragmentation process to study hyperfine interactions. We have measured the magnetic moments of mirror nuclei using this method at the Lawrence Berkeley Laboratory's Bevalac heavy-ion accelerator. We present the merits, applicability and limitations of the technique.

    DOI: 10.1007/BF00567486

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  • NMR LINE-WIDTH OF B-12 IN PT DETECTED BY BETA-NMR Reviewed

    T OHTSUBO, K MATSUDA, T ARAKI, M MORI, M FUKUDA, K MATSUTA, Y NOJIRI, T MINAMISONO

    HYPERFINE INTERACTIONS   78 ( 1-4 )   439 - 443   1993

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    NMR spectra of B-12 in Pt (fcc) metal were observed by use of the beta-NMR detection method. A sharp single line was observed by use of an annealed Pt foil for the implantation medium. The dipolar broadening has been determined to be 332 +/- 30 Hz (HWHM).

    DOI: 10.1007/BF00568171

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  • NEW NUCLEAR-QUADRUPOLE RESONANCE TECHNIQUE IN BETA-NMR Reviewed

    T MINAMISONO, T OHTSUBO, S FUKUDA, MINAMI, I, Y NAKAYAMA, M FUKUDA, K MATSUTA, Y NOJIRI

    HYPERFINE INTERACTIONS   80 ( 1-4 )   1315 - 1319   1993

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    The beta-NMR technique has been modified in order to detect efficiently the nuclear quadrupole effects in the NMR spectra. Beta-NMR is detected as a function of coupling frequency; all RFs that correspond to the coupling frequency were applied simultaneously.

    DOI: 10.1007/BF00567497

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  • PRECISE MEASUREMENT OF THE MAGNETIC-MOMENT OF DOUBLY CLOSED SHELL+1 NUCLEON-NUCLEUS F-17(I-PI=5/2+,T1/2=64.5S) Reviewed

    T MINAMISONO, T OHTSUBO, S FUKUDA, Y NAKAYAMA, T ARAKI, K MASITANI, K MATSUDA, E TAKAHASHI, M TANIGAKI, M TANAKA, H SHIOHARA, Y SOMEDA, Y AOKI, A KITAGAWA, M FUKUDA, K MATSUTA, Y NOJIRI

    HYPERFINE INTERACTIONS   78 ( 1-4 )   111 - 116   1993

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    Hyperfine interactions of beta-emitting F-17 implanted in single crystals of NaF and CaF2 were studied. The nuclear magnetic moment of the I(pi) = 5/2+ state was determined with improved precision to be \mu(F-17; I(pi) = 5/2+, T1/2 = 64.5 s)\ = 4.72130 +/- 0.00025 mu(N).

    DOI: 10.1007/BF00568124

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  • BETA-NMR DETECTION OF BETA-EMITTING FRAGMENT TI-43 Reviewed

    K MATSUTA, A OZAWA, Y NOJIRI, T MINAMISONO, M FUKUDA, S MOMOTA, T OHTSUBO, S FUKUDA, K SUGIMOTO, TANIHATA, I, K YOSHIDA, K OMATA, ALONSO, JR, GF KREBS, TJM SYMONS

    HYPERFINE INTERACTIONS   78 ( 1-4 )   123 - 126   1993

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    NMR on the beta emitter Ti-43 has been observed by use of the beta-NMR technique. From the observed NMR spectrum, the magnetic moment of Ti-43 was determined to be Absolute value of mu = 0.85 +/- 0.02 mu(N). The value is significantly quenched from the single particle value -1.91 mu(N), which shows a strong effect resulting from meson-exchange currents and configuration mixing.

    DOI: 10.1007/BF00568126

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  • HYPERFINE INTERACTIONS OF B-12 IN BN (HEXAGONAL) Reviewed

    T OHTSUBO, M TANIGAKI, S FUKUDA, Y NAKAYAMA, S TAKEDA, N NAKAMURA, H TANJI, M FUKUDA, K MATSUTA, Y NOJIRI, T MINAMISONO

    HYPERFINE INTERACTIONS   78 ( 1-4 )   185 - 190   1993

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    Hyperfine interactions of B-12(I(pi) = 1+, T1/2 = 21 ms) implanted in the substitutional site of B in BN (hexagonal) was studied by detecting beta-NMR. In order to measure the quadrupole coupling constant efficiently, we employed a newly developed quadrupole resonance technique (NNQR). The quadrupole moment of B-12 was determined to be \Q(B-12)\ = 13.21 +/- 0.26 mb.

    DOI: 10.1007/BF00568137

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  • NEW DETERMINATION OF QUADRUPOLE COUPLING-CONSTANTS OF LI ISOTOPES IN SINGLE-CRYSTALS LIIO3 AND LINBO3 Reviewed

    T MINAMISONO, T OHTSUBO, Y NAKAYAMA, S FUKUDA, T IZUMIKAWA, M TANIGAKI, M MATSUI, S TAKEDA, N NAKAMURA, M FUKUDA, K MATSUTA, Y NOJIRI

    HYPERFINE INTERACTIONS   78 ( 1-4 )   159 - 163   1993

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    Quadrupole effects in NMR spectra of Li-8(I(pi) = 2+; T1/2 = 0.84 s) in LiIO3 and LiNbO3 single crystals have been detected by use of a modified beta-NMR. The coupling constants for both crystals are in agreement with known ones. Field gradients in the crystals were measured by detecting pulsed-Fourier transformed NMR of Li-7. The quadrupole moments deduced from both samples agree, and \Q(Li-8; 2+)\ = 32.7 +/- 0.6 mb has been determined.

    DOI: 10.1007/BF00568132

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  • PRECISE MEASUREMENT OF THE MAGNETIC-MOMENT OF DOUBLY CLOSED SHELL-1 NUCLEON-NUCLEUS O-15(I-PI=1/2-,T1/2=122S) Reviewed

    M TANIGAKI, M MATSUI, M MIHARA, M MORI, M TANAKA, T YANAGISAWA, T OHTSUBO, T IZUMIKAWA, A KITAGAWA, M FUKUDA, K MATSUTA, Y NOJIRI, T MINAMISONO

    HYPERFINE INTERACTIONS   78 ( 1-4 )   105 - 110   1993

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    The magnetic moment of O-15(I(pi) = 1/2-, T1/2 = 122 s) has been measured precisely by use of the beta-NMR detection of O-15 in TiO2 as, \mu(O-15; 1/2-)\ = 0.71951(12) mu(N). The effective nucleon mass in the nuclei around mass number 16 was discussed using the isoscalar moment deduced in connection with the magnetic moment of N-15.

    DOI: 10.1007/BF00568123

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  • PRECISE MEASUREMENT OF QUADRUPOLE-MOMENT OF B-8 BY USE OF A MODIFIED BETA-NMR Reviewed

    T MINAMISONO, T OHTSUBO, MINAMI, I, S FUKUDA, A KITAGAWA, Y NAKAYAMA, M FUKUDA, K MATSUTA, Y NOJIRI

    HYPERFINE INTERACTIONS   78 ( 1-4 )   169 - 173   1993

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    The nuclear quadrupole moment of B-8(I(pi) = 2+, T1/2 = 769 ms) has been determined by use of a modified beta-NMR detection as \Q(B-8)\ = 68.3 +/- 2.1 mb. A field gradient was obtained in a single crystal Mg at room temperature.

    DOI: 10.1007/BF00568134

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  • MAGNETIC-MOMENT OF MG-23 Reviewed

    M FUKUDA, T IZUMIKAWA, T OHTSUBO, M TANIGAKI, S FUKUDA, Y NAKAYAMA, K MATSUTA, Y NOJIRI, T MINAMISONO

    HYPERFINE INTERACTIONS   78 ( 1-4 )   117 - 121   1993

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    The magnetic moment of the Mg-23 (I(pi) = 3/2+, T1/2 = 11.3 s), has been determined as \mu(Mg-23)\ = 0.5364 +/- 0.0003 mu(N) by use of beta-NMR detection with the recoil polarization obtained through a low energy nuclear reaction.

    DOI: 10.1007/BF00568125

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  • PRODUCTION AND POLARIZATION OF BETA-EMITTING PROJECTILE FRAGMENT TI-43 Reviewed

    K MATSUTA, A OZAWA, Y NOJIRI, T MINAMISONO, M FUKUDA, S MOMOTA, T OHTSUBO, S FUKUDA, K SUGIMOTO, TANIHATA, I, K YOSHIDA, K OMATA, ALONSO, JR, GF KREBS, TJM SYMONS

    PROCEEDINGS OF THE THIRD INTERNATIONAL CONFERENCE ON RADIOACTIVE NUCLEAR BEAMS   377 - 381   1993

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  • QUADRUPOLE-MOMENT OF SC-41 BY USE OF NEW NUCLEAR-QUADRUPOLE RESONANCE DETECTION Reviewed

    T MINAMISONO, S FUKUDA, T OHTSUBO, M TANIGAKI, A KITAGAWA, M FUKUDA, K MATSUTA, Y NOJIRI, S TAKEDA

    HYPERFINE INTERACTIONS   78 ( 1-4 )   191 - 194   1993

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    Quadrupole effects in beta-NMR spectra of Sc-41(I(pi) = 7/2-, T1/2 = 0.596 s) implanted in a TiO2 single crystal were detected by use of a modified beta-NMR technique. Using the field gradient in the crystal determined by the pulsed-Fourier-transformed NMR of Sc-45 in TiO2, the quadrupole moment of Sc-41 has been determined as \Q(Sc-41; 7/2-)\ = 166 +/- 8 mb.

    DOI: 10.1007/BF00568138

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  • GIANT QUADRUPOLE-MOMENT AND PROTON HALO DISCOVERED IN B-8 Reviewed

    T MINAMISONO, T OHTSUBO, MINAMI, I, A KITAGAWA, S FUKUDA, Y NAKAYAMA, M FUKUDA, K MATSUTA, Y NOJIRI, S TAKEDA, H SAGAWA, H KITAGAWA

    HYPERFINE INTERACTIONS   78 ( 1-4 )   165 - 168   1993

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    The nuclear quadrupole moment of B-8(I(pi) = 2+, T1/2 = 769 ms) has been determined by use of a modified beta-NMR detection as \Q(B-8)\ = 68.3 +/- 2.1 mb, which is twice the prediction of the Cohen-Kurath shell model calculation. The anomalous quadrupole moment which is carried mainly by the protons in the nucleus, has been accounted for by the proton halo effect.

    DOI: 10.1007/BF00568133

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  • NMR ON BETA-EMITTING FRAGMENT TI-43 Reviewed

    K MATSUTA, A OZAWA, Y NOJIRI, T MINAMISONO, M FUKUDA, S MOMOTA, T OHTSUBO, S FUKUDA, K SUGIMOTO, TANIHATA, I, K YOSHIDA, K OMATA, ALONSO, JR, GF KREBS, TJM SYMONS

    NUCLEI FAR FROM STABILITY/ATOMIC MASSES AND FUNDAMENTAL CONSTANTS 1992   ( 132 )   229 - 231   1993

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    NMR has been observed on beta-emitting Ti-43 produced in the 116 AMeV Ti-46 On C collision by means of asymmetric beta decay. The observed spin polarization of Ti-43 showed a reversed tendency in its momentum dependence compared with that observed for fragments produced in the Ca-40 on Au collision. This suggests negative angle deflection of Ti-43 due to the nuclear attractive potential. From the observed NMR spectrum, the magnetic moment of Ti-43 was determined to be \mu\=(0.85 +/- 0.02) mu(N). The value is significantly quenched from the single particle value -1.91 mu(N), which shows a strong effect due to meson exchange currents and configuration mixing.

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  • FRAGMENT POLARIZATION OF TI-43 IN THE TI-46+C COLLISION Reviewed

    K MATSUTA, A OZAWA, Y NOJIRI, T MINAMISONO, M FUKUDA, S MOMOTA, T OHTSUBO, S FUKUDA, K SUGIMOTO, TANIHATA, I, K YOSHIDA, K OMATA, ALONSO, JR, GF KREBS, TJM SYMONS

    HYPERFINE INTERACTIONS   78 ( 1-4 )   127 - 131   1993

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    Spin polarization of Ti-43 produced through the projectile fragmentation process in Ti-46 on C collisions at 116 MeV/nucleon has been observed as a function of fragment momentum by means of beta-decay asymmetry. From the momentum dependence of the fragment polarization, it was concluded that negative angle deflection of the Ti-43 fragment due to the nuclear attractive potential is the main reaction path in the case of light targets.

    DOI: 10.1007/BF00568127

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  • A FRAGMENT SEPARATOR AT LBL FOR THE BETA-NMR EXPERIMENT Reviewed

    K MATSUTA, A OZAWA, Y NOJIRI, T MINAMISONO, M FUKUDA, A KITAGAWA, T OHTSUBO, S MOMOTA, S FUKUDA, Y MATSUO, H TAKECHI, MINAMI, I, K SUGIMOTO, TANIHATA, I, K OMATA, S SHIMOURA, ALONSO, JR, GF KREBS, TJM SYMONS

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B-BEAM INTERACTIONS WITH MATERIALS AND ATOMS   70 ( 1-4 )   304 - 308   1992.8

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    The Beam 44 fragment separator was built at the Bevalac of LBL for NMR studies of beta emitting nuclei. K-37, Ca-39, and Ti-43 fragments originating from Ca-40 and Ti-46 primary beams were separated by the separator for NMR studies on these nuclei. Nuclear spin polarization was created in Ca-39 and Ti-43 using the tilted foil technique (TFT), and the magnetic moment of Ti-43 was deduced. Fragment polarization was measured for K-37 and Ca-39 emitted to finite deflection angles. The Beam 44 fragment separator in combination with a proper polarization technique, such as TFT or fragment polarization, has been very effective for such NMR studies.

    DOI: 10.1016/0168-583X(92)95946-O

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  • POLARIZATION PHENOMENA IN PROJECTILE FRAGMENTATION PROCESS Reviewed

    K MATSUTA, A OZAWA, Y NOJIRI, T MINAMISONO, M FUKUDA, A KITAGAWA, S MOMOTA, T OHTSUBO, Y MATSUO, H TAKECHI, S FUKUDA, MINAMI, I, K SUGIMOTO, TANIHATA, I, K OMATA, ALONSO, JR, GF KREBS, TJM SYMONS

    RADIOACTIVE NUCLEAR BEAMS 1991   361 - 366   1992

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  • NMR ON SHORT-LIVED BETA-EMITTER TI-43 USING NEW FRAGMENT SEPARATOR AT LBL Reviewed

    K MATSUTA, M IZUMI, A KITAGAWA, Y NOJIRI, T MINAMISONO, A OZAWA, T OHTSUBO, S MOMOTA, Y MATSUO, K SUGIMOTO, K OMATA, Y SHIDA, TANIHATA, I, S SHIMOURA, T KOBAYASHI, ALONSO, JR, GF KREBS, TJM SYMONS

    HYPERFINE INTERACTIONS   61 ( 1-4 )   1387 - 1390   1990.8

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    DOI: 10.1007/BF02407632

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  • Deeply bound pionic 1s states in Sn isotopes

    K Suzuki, M Fujita, H Geissel, H Gilg, A Gillitzer, RS Hayano, S Hirenzaki, K Itahashi, M Iwasaki, P Kienle, M Matos, G Munzenberg, T Ohtsubo, M Sato, M Shindo, T Suzuki, H Weick, M Winkler, T Yamazaki, T Yoneyama

    NUCLEAR PHYSICS A   721   831C - 834C   2003.6

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    We successfully observed deeply bound picnic 1s states in Sn isotopes (Sn-115, Sn-119, Sn-123) using the Sn(d,He-3) pion-transfer reaction under the recoil-free condition. The 1s binding energies and widths were determined to high precision. The present results indicate that the isovector part of the s-wave pion-nucleus interaction is significantly enhanced, giving a clear evidence for partial restoration of chiral symmetry in the nuclear medium.

    DOI: 10.1016/S0375-9474(03)01219-3

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  • Deeply bound pionic 1s states in Sn isotopes

    K Suzuki, M Fujita, H Geissel, H Gilg, A Gillitzer, RS Hayano, S Hirenzaki, K Itahashi, M Iwasaki, P Kienle, M Matos, G Munzenberg, T Ohtsubo, M Sato, M Shindo, T Suzuki, H Weick, M Winkler, T Yamazaki, T Yoneyama

    NUCLEAR PHYSICS A   721   831C - 834C   2003.6

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    We successfully observed deeply bound picnic 1s states in Sn isotopes (Sn-115, Sn-119, Sn-123) using the Sn(d,He-3) pion-transfer reaction under the recoil-free condition. The 1s binding energies and widths were determined to high precision. The present results indicate that the isovector part of the s-wave pion-nucleus interaction is significantly enhanced, giving a clear evidence for partial restoration of chiral symmetry in the nuclear medium.

    DOI: 10.1016/S0375-9474(03)01219-3

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  • Energy and range focusing of in-flight separated exotic nuclei - A study for the energy-buncher stage of the low-energy branch of the Super-FRS

    C Scheidenberger, H Geissel, M Maier, G Munzenberg, M Portillo, G Savard, P Van Duppen, H Weick, M Winkler, M Yavor, F Attallah, KH Behr, Chichkine, V, S Eliseev, M Hausmann, M Hellstrom, E Kaza, B Kindler, Y Litvinov, B Lommel, G Marx, M Matos, N Nankov, T Ohtsubo, K Summerer, ZY Sun, Z Zhou

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B-BEAM INTERACTIONS WITH MATERIALS AND ATOMS   204   119 - 123   2003.5

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    The relative momentum spread of in-flight separated exotic nuclear beams produced in fragmentation and/or fission reactions is of the order of a few percent. A new technique is presented, which reduces the momentum spread significantly, and first experimental results obtained with relativistic projectile fragments are shown. This technique is the key to experiments with slowed-down and stopped beams, in particular for the efficient stopping of relativistic exotic nuclei in gas-filled stopping cells. It will be employed at the energy-buncher stage of the low-energy branch of the Super-FRS facility. The ion-optical design of the energy buncher is presented and a brief outlook to the experimental program is given. (C) 2002 Elsevier Science B.V. All rights reserved.

    DOI: 10.1016/S0168-583X(02)01898-0

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  • Energy and range focusing of in-flight separated exotic nuclei - A study for the energy-buncher stage of the low-energy branch of the Super-FRS

    C Scheidenberger, H Geissel, M Maier, G Munzenberg, M Portillo, G Savard, P Van Duppen, H Weick, M Winkler, M Yavor, F Attallah, KH Behr, Chichkine, V, S Eliseev, M Hausmann, M Hellstrom, E Kaza, B Kindler, Y Litvinov, B Lommel, G Marx, M Matos, N Nankov, T Ohtsubo, K Summerer, ZY Sun, Z Zhou

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B-BEAM INTERACTIONS WITH MATERIALS AND ATOMS   204   119 - 123   2003.5

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    Language:English   Publisher:ELSEVIER SCIENCE BV  

    The relative momentum spread of in-flight separated exotic nuclear beams produced in fragmentation and/or fission reactions is of the order of a few percent. A new technique is presented, which reduces the momentum spread significantly, and first experimental results obtained with relativistic projectile fragments are shown. This technique is the key to experiments with slowed-down and stopped beams, in particular for the efficient stopping of relativistic exotic nuclei in gas-filled stopping cells. It will be employed at the energy-buncher stage of the low-energy branch of the Super-FRS facility. The ion-optical design of the energy buncher is presented and a brief outlook to the experimental program is given. (C) 2002 Elsevier Science B.V. All rights reserved.

    DOI: 10.1016/S0168-583X(02)01898-0

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  • High-energy breakup of <sup>8</sup>B (共著)

    Nuclear Physics A   718, 431   2003

  • Nuclear magnetic resonance on oriented nuclei of <sup>91</sup>SrFe (共著)

    Physical Review B   68, 012403   2003

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  • Nuclear and Coulmb breakup of <sup>8</sup>B (共著)

    Nuclear Physics A   720, 3   2003

  • Nuclear and Coulmb breakup of <sup>8</sup>B (共著)

    Nuclear Physics A   720, 3   2003

  • High-energy breakup of <sup>8</sup>B (共著)

    Nuclear Physics A   718, 431   2003

  • Nuclear magnetic resonance on oriented nuclei of <sup>91</sup>SrFe (共著)

    Physical Review B   68, 012403   2003

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  • Nuclear spin relaxation of extremely dilute impurities using brute-force NMRON

    K Nishimura, S Ohya, Y Kawamura, T Ohtsubo, T Izumikawa, S Muto, K Mori

    JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN   71 ( 6 )   1589 - 1593   2002.6

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    Brute-force nuclear magnetic resonance on oriented nuclei (BF-NMRON) was used to investigate the nuclear spin-relaxation times, T-1, of Nb-90 in Nb and Cu, Tc-96 in Nb, Rh-101m in Cu, and I Ag-101m in Ag with an external field of 11.922 T at about 10 mK. The observed relaxation times with known nuclear g-factors were used to estimate the converted relaxation rates, (T(1)Tg(n)(2))(-1), which were compared with those n obtained from NMR and other methods. From the comparison, it was found that (T-1 Tg(n)(2))(-1) of Nb-90 in Nb n and Ag-110m in Ag coincided with those of the bulk systems. (T-1 Tg(n)(2))(-1) of Nb-90 in CU Was about four times n larger than that of Nb bulk system. Both Tc-96 in Nb and Rh-101m in Cu produced (T(1)Tg(n)(2))(-1) values n consistent with previous studies.

    DOI: 10.1143/JPSJ.71.1589

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  • Nuclear spin relaxation of extremely dilute impurities using brute-force NMRON

    K Nishimura, S Ohya, Y Kawamura, T Ohtsubo, T Izumikawa, S Muto, K Mori

    JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN   71 ( 6 )   1589 - 1593   2002.6

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    Brute-force nuclear magnetic resonance on oriented nuclei (BF-NMRON) was used to investigate the nuclear spin-relaxation times, T-1, of Nb-90 in Nb and Cu, Tc-96 in Nb, Rh-101m in Cu, and I Ag-101m in Ag with an external field of 11.922 T at about 10 mK. The observed relaxation times with known nuclear g-factors were used to estimate the converted relaxation rates, (T(1)Tg(n)(2))(-1), which were compared with those n obtained from NMR and other methods. From the comparison, it was found that (T-1 Tg(n)(2))(-1) of Nb-90 in Nb n and Ag-110m in Ag coincided with those of the bulk systems. (T-1 Tg(n)(2))(-1) of Nb-90 in CU Was about four times n larger than that of Nb bulk system. Both Tc-96 in Nb and Rh-101m in Cu produced (T(1)Tg(n)(2))(-1) values n consistent with previous studies.

    DOI: 10.1143/JPSJ.71.1589

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  • Nuclear spin relaxation of extremely dilute impurities using Brute-Force NMRON (共著)

    J. Phys. Soc. Jpn.   71, 1589   2002

  • Recent studies on the nuclear moments of light mirror nuclei (T = 1/2, 3/2) (共著)

    Nuclear Physics A   704, 98   2002

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  • Recent studies on the nuclear moments of light mirror nuclei (T = 1/2, 3/2) (共著)

    Nuclear Physics A   704, 98   2002

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  • Nuclear magnetic moment of the <sup>143</sup>Ce ground state (共著)

    Physcal Revew C   65, 017301   2002

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  • Precise magnetic moment of short-lived beta emitter <sup>35</sup>Ar (共著)

    Nuclear Physics A   701, 383   2002

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  • Experimental evidence for the <sup>8</sup>B ground state configuration (共著)

    Phys. Lett. B   529, 36   2002

  • Experimental evidence for the <sup>8</sup>B ground state configuration (共著)

    Phys. Lett. B   529, 36   2002

  • Measurements of the interaction cross sections for Ar and Cl isotopes (共著)

    Nuclear Physics A   709, 60   2002

  • Measurements of the interaction cross sections for Ar and Cl isotopes (共著)

    Nuclear Physics A   709, 60   2002

  • Precise magnetic moment of short-lived beta emitter <sup>35</sup>Ar (共著)

    Nuclear Physics A   701, 383   2002

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  • Nuclear magnetic moment of the <sup>143</sup>Ce ground state (共著)

    Physcal Revew C   65, 017301   2002

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  • Nuclear spin relaxation of extremely dilute impurities using Brute-Force NMRON (共著)

    J. Phys. Soc. Jpn.   71, 1589   2002

  • Progress in Mass Measurements of Stored Exotic Nuclei at Relativistic Energies (共著)

    Nucl. Phys. A   685, 115c   2001

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  • Brute-force NMR-ON on 90NbCu, 101mRhCu and 110mAgAg

    S. Ohya, Y. Izubuchi, J. Goto, T. Ohtsubo, S. Muto, K. Nishimura

    Hyperfine Interactions   133 ( 1-4 )   105 - 109   2001

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    Brute-force nuclear magnetic resonance on oriented nuclei (BF-NMRON) experiments have been performed for 90NbCu, 101mRhCu and 110mAgAg at about 10 mK. Narrow resonance spectra were detected. Using the known values of the g-factors, the Knight shift has been deduced: K(90NbCu) = 0.62(24) %, K(101mRhCu) = 0.87(27)%. The effective spin-lattice relaxation times were also measured.

    DOI: 10.1023/A:1012213519149

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  • The Hyperfine Field of Selenium in Iron and the Magnetic Dipole Moment of <sup>75</sup>Se (共著)

    Hyperfine Interactions   133, 117   2001

  • Magneti hyperfine fields of <sup>151</sup>PmFe and <sup>147</sup>NdNi (共著)

    Hyperfine Interactions   136 ( 137 )   561   2001

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  • Brute-force NMR-ON on 90NbCu, 101mRhCu and 110mAgAg

    S. Ohya, Y. Izubuchi, J. Goto, T. Ohtsubo, S. Muto, K. Nishimura

    Hyperfine Interactions   133 ( 1-4 )   105 - 109   2001

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    Language:English  

    Brute-force nuclear magnetic resonance on oriented nuclei (BF-NMRON) experiments have been performed for 90NbCu, 101mRhCu and 110mAgAg at about 10 mK. Narrow resonance spectra were detected. Using the known values of the g-factors, the Knight shift has been deduced: K(90NbCu) = 0.62(24) %, K(101mRhCu) = 0.87(27)%. The effective spin-lattice relaxation times were also measured.

    DOI: 10.1023/A:1012213519149

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  • The Hyperfine Field of Selenium in Iron and the Magnetic Dipole Moment of <sup>75</sup>Se (共著)

    Hyperfine Interactions   133, 117   2001

  • Progress in Mass Measurements of Stored Exotic Nuclei at Relativistic Energies (共著)

    Nucl. Phys. A   685, 115c   2001

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  • Magneti hyperfine fields of <sup>151</sup>PmFe and <sup>147</sup>NdNi (共著)

    Hyperfine Interactions   136 ( 137 )   561   2001

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  • Knight shift of Nb-90, Mo-93m, Tc-96, and Rh-101m in Nb using brute-force NMRON

    K Nishimura, S Ohya, Y Kawamura, T Ohtsubo, T Izumikawa, S Muto

    HYPERFINE INTERACTIONS   136 ( 137 )   567 - 572   2001

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    Brute-force nuclear magnetic resonance on oriented nuclei (BF-NMRON) of Nb-90, Mo-93m, Tc-96, and Rh-101m was carried out in a new host metal, Nb. The resonance center frequencies at an external field of 11.922(6) T were obtained as v((NbNb)-Nb-90) = 56.572(9) MHz, v((MoNb)-Mo-93m) = 85.76(3) MHz, v((TcNb)-Tc-96) = 66.997(11) MHz, and v(Rh-101m Nb) = 111.010(19) MHz. A systematic analysis of the Knight shift of 4d elements in extremely dilute alloy systems is briefly discussed.

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  • Isochronous Mass Measurement of Hot Exotic Nuclei (共著)

    Hyperfine Interactions   132, 291   2001

  • Isochronous Mass Measurement of Hot Exotic Nuclei (共著)

    Hyperfine Interactions   132, 291   2001

  • Knight shift of Nb-90, Mo-93m, Tc-96, and Rh-101m in Nb using brute-force NMRON

    K Nishimura, S Ohya, Y Kawamura, T Ohtsubo, T Izumikawa, S Muto

    HYPERFINE INTERACTIONS   136 ( 137 )   567 - 572   2001

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    Brute-force nuclear magnetic resonance on oriented nuclei (BF-NMRON) of Nb-90, Mo-93m, Tc-96, and Rh-101m was carried out in a new host metal, Nb. The resonance center frequencies at an external field of 11.922(6) T were obtained as v((NbNb)-Nb-90) = 56.572(9) MHz, v((MoNb)-Mo-93m) = 85.76(3) MHz, v((TcNb)-Tc-96) = 66.997(11) MHz, and v(Rh-101m Nb) = 111.010(19) MHz. A systematic analysis of the Knight shift of 4d elements in extremely dilute alloy systems is briefly discussed.

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  • Electromagnetic moments of short lived β emitters <sup>21</sup>F, <sup>23</sup>Mg, <sup>27</sup>Si and <sup>39</sup>Ca

    Hyperfine Interactions (共著)   120-121, 673   1999

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  • Magnetic hyperfine interaction of Br in Ni (共著)

    Hyperfine Interactions   120-121   1999

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  • Magnetic hyperfine field of Hg in Nickel and the sigh of magnetic moment of <sup>197m</sup>Au by NMR-ON (共著)

    Hyperfine Interactions   120-121, 683   1999

  • Polarized beam of unstable nuclei via ion beam surface interaction at grazing incidence (共著)

    Hyperfine Interactions   120-121, 695   1999

  • Polarized beam of unstable nuclei via ion beam surface interaction at grazing incidence (共著)

    Hyperfine Interactions   120-121, 695   1999

  • Magnetic moments of <sup>76</sup>As and <sup>77</sup>As (共著)

    Phys. Rev. C   59, 669   1999

  • Magnetic moments of <sup>76</sup>As and <sup>77</sup>As (共著)

    Phys. Rev. C   59, 669   1999

  • Quadrupole moment of the proton drip-line nuclide <sup>13</sup>O (共著)

    Physics Letters B   459, 81   1999

  • Quadrupole moment of the proton drip-line nuclide <sup>13</sup>O (共著)

    Physics Letters B   459, 81   1999

  • Knight shifts for short-lived β emitters in Pt (共著)

    Hyperfine Interactions   120-121, 719   1999

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  • Density distribution of <sup>8</sup>B studied via reaction cross sections (共著)

    Nuclear Physics A   656, 209   1999

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  • Electromagnetic moments of short lived β emitters <sup>21</sup>F, <sup>23</sup>Mg, </sup>27</sup>Si and </sup>39</sup>Ca

    Hyperfine Interactions (共著)   120-121, 673   1999

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  • Spin polarization of β-emitting fragments in high energy heavy ions on Be collisions

    Hyperfine Interactions (共著)   120-121, 713   1999

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  • Magnetic hyperfine field of Hg in Nickel and the sigh of magnetic moment of <sup>197m</sup>Au by NMR-ON (共著)

    Hyperfine Interactions   120-121, 683   1999

  • Density distribution of <sup>8</sup>B studied via reaction cross sections (共著)

    Nuclear Physics A   656, 209   1999

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  • Spin polarization of β-emitting fragments in high energy heavy ions on Be collisions

    Hyperfine Interactions (共著)   120-121, 713   1999

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  • Knight shifts for short-lived β emitters in Pt (共著)

    Hyperfine Interactions   120-121, 719   1999

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  • Magnetic hyperfine interaction of Br in Ni (共著)

    Hyperfine Interactions   120-121   1999

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  • Quadrupole morment of the proton rich β-emitting nucleus <sup>12</sup>N

    MINAMISONO T, OHTSUBO T, SATO K, TAKEDA S, FUKUDA S, IZUMIKAWA T, TANIGAKI M, TANJI H, NOJIRI Y

    Physics Letters B   420 ( 1/2 )   31 - 36   1998

  • Quadrupole morment of the proton rich β-emitting nucleus <sup>12</sup>N

    Physics Letters B   420 ( 1/2 )   31 - 36   1998

  • Measurements for spin inversion and noninversion in successive decays via nuclear magnetic resonance on oriented nuclei

    S Ohya, T Ohtsubo, K Komatsuzaki, DJ Cho, S Muto

    PHYSICAL REVIEW C   54 ( 3 )   1129 - 1132   1996.9

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    Language:English   Publisher:AMERICAN PHYSICAL SOC  

    Nuclear magnetic resonance on oriented nuclei (NMR-ON) measurements were performed on the successive decays of Zr-89-Y-89(m) and Os-191-Ir-191(m) in Fe. The NMR-ON spectra of (ZrFe)-Zr-89 and (OsFe)-Os-191 were obtained by detecting gamma rays from the decay of the isomers, Y-89(m) and Ir-191(m), respectively. For (ZrFe)-Zr-89, the anisotropy of the gamma ray increased at the resonance. On the other hand, for (OsFe)-Os-191 the anisotropy of the gamma ray decreased at the resonance. These phenomena were explained using the spin inversion and spin noninversion processes including the lifetimes of the isomers and spin lattice relaxation times. NMR-ON measurements for such spin inversion and noninversion processes were reported. The resonance spectra were also observed by detecting beta rays from Zr-89 and Os-191. In these experiments the magnetic moments of Zr-89 and Os-191 were determined to be -1.08 (2) mu(N) and 0.962 (28) mu(N), respectively. The signs of the magnetic moments of Y-89(m) and Ir-191(m) were also determined to be positive.

    DOI: 10.1103/PhysRevC.54.1129

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  • Measurements for spin inversion and noninversion in successive decays via nuclear magnetic resonance on oriented nuclei

    S Ohya, T Ohtsubo, K Komatsuzaki, DJ Cho, S Muto

    PHYSICAL REVIEW C   54 ( 3 )   1129 - 1132   1996.9

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    Nuclear magnetic resonance on oriented nuclei (NMR-ON) measurements were performed on the successive decays of Zr-89-Y-89(m) and Os-191-Ir-191(m) in Fe. The NMR-ON spectra of (ZrFe)-Zr-89 and (OsFe)-Os-191 were obtained by detecting gamma rays from the decay of the isomers, Y-89(m) and Ir-191(m), respectively. For (ZrFe)-Zr-89, the anisotropy of the gamma ray increased at the resonance. On the other hand, for (OsFe)-Os-191 the anisotropy of the gamma ray decreased at the resonance. These phenomena were explained using the spin inversion and spin noninversion processes including the lifetimes of the isomers and spin lattice relaxation times. NMR-ON measurements for such spin inversion and noninversion processes were reported. The resonance spectra were also observed by detecting beta rays from Zr-89 and Os-191. In these experiments the magnetic moments of Zr-89 and Os-191 were determined to be -1.08 (2) mu(N) and 0.962 (28) mu(N), respectively. The signs of the magnetic moments of Y-89(m) and Ir-191(m) were also determined to be positive.

    DOI: 10.1103/PhysRevC.54.1129

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  • Hyperfine interaction of <sup>13</sup>O and <sup>23</sup>Mg implanted in Pt(共著)

    Hyperfine Interactions   97 ( 98/ )   501   1996

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  • Magnetic Moments of proton drip-line <sup>13</sup> O and <sup>9</sup>C (共著)

    Hyperfine Interactions   97 ( 98/ )   519   1996

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  • Measurement of the nuclear magnetic moments of <sup>57</sup>Ni and <sup>59</sup>Fe(共著)

    Physical Review C   54,554   1996

  • Hyperfine interaction of <sup>13</sup>O and <sup>23</sup>Mg implanted in Pt(共著)

    Hyperfine Interactions   97 ( 98/ )   501   1996

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  • Measurement of the nuclear magnetic moments of <sup>57</sup>Ni and <sup>59</sup>Fe(共著)

    Physical Review C   54 ( 2 )   554 - 558   1996

  • Magnetic Moments of proton drip-line <sup>13</sup>O and <sup>9</sup>C (共著)

    Hyperfine Interactions   97 ( 98/ )   519   1996

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  • Precise measurement of the quadruple moment of β-emitting <sup>12</sup>B(共著)

    Hyperfine Interactions   88   25   1994

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  • Precise measurement of the quadruple moment of β-emitting <sup>12</sup>B(共著)

    Hyperfine Interactions   88   25   1994

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  • Magnetic moment of <sup>23</sup>Mg(共著)

    Hyperfine Interactions   78,117   1993

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  • Magnetic moment of the short-lived β-emitting <sup>23</sup>Mg(共著)

    Physics Letters B   307,278   1993

  • Magnetic moment of the short-lived β-emitting <sup>23</sup>Mg(共著)

    Physics Letters B   307,278   1993

  • Quadrupole moment of the doubly-closed-shell-plus-one-nucleon nucleus <sup>41</sup>Sc and its core deformation(共著)

    Nuclear Physics A   559,239   1993

  • Quadrupole moment of the doubly-closed-shell-plus-one-nucleon nucleus <sup>41</sup>Sc and its core deformation(共著)

    Nuclear Physics A   559,239   1993

  • Quadrupole interactions of Li isotopes in single crystal LiIO<sub>3</sub> and LiNbO<sub>3</sub> - Problem solved - (共著)

    Hyperfine Interactions   78, 159   1993

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  • Giant quadrupole moment and proton halo discovered in <sup>8</sup>B(共著)

    Hyperfine Interactions   78,165   1993

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  • Precise measurement of quadrupole moment of <sup>8</sup>B by use of a modified β-NMR(共著)

    Hyperfine Interactions   78,169   1993

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  • Precise measurement of the magnetic moment of doubly closed shell+1 nucleon neacleus <sup>17</sup>F(I<sup>π=5/2<sup>+</sup>, T<sub>1/2</sub>=64.5s)(共著)

    Hyperfine Interactions   78,111   1993

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  • Beta-NMR detection of beta-emitting fragment <sup>43</sup>Ti(共著)

    Hyperfine Interactions   78,123   1993

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  • Fragment polarization of <sup>43</sup>Ti in the <sup>46</sup>Ti+C collision(共著)

    Hyperfine Interactions   78,127   1993

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  • NMR line width of <sup>12</sup> in Pt detected by β-NMR(共著)

    Hyperfine Interactions   78,439   1993

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  • Quadrupole moment of <sup>41</sup>Sc by use of new nuclear quadrupole resonance detection(共著)

    Hyperfine Interactions   78,191   1993

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  • Precise measurement of the magnetic moment of doubly closed shell-1 nucleon nucleus <sup>15</sup>O(I<sup>π</sup>=1/2<sup>-</sup>, T<sub>1/2</sub>=122sec)(共著)

    Hyperfine Interactions   78,105   1993

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  • Hyperfine interactions of <sup>12</sup>B in BN(hexagonal)(共著)

    Hyperfine Interactions   78,185   1993

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  • Quadrupole interactions of Li isotopes in single crystal LiIO<sub>3</sub> and LiNbO<sub>3</sub> - Problem solved - (共著)

    Hyperfine Interactions   78, 159   1993

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  • Giant quadrupole moment and proton halo discovered in <sup>8</sup>B nucleus(共著)

    Hyperfine Interactions   78,165   1993

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  • Precise measurement of quadrupole moment of <sup>8</sup>B by use of a modified β-NMR(共著)

    Hyperfine Interactions   78,169   1993

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  • Precise measurement of the magnetic moment of doubly closed shell+1 nucleon neacleus <sup>17</sup>F(I<sup>π</sup>=5/2<sup>+</sup>, T<sub>1/2</sub>=64.5sec)(共著)

    Hyperfine Interactions   78,111   1993

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  • Beta-NMR detection of beta-emitting fragment <sup>43</sup>Ti(共著)

    Hyperfine Interactions   78,123   1993

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  • Fragment polarization of <sup>43</sup>Ti in the <sup>46</sup>Ti+C collision(共著)

    Hyperfine Interactions   78,127   1993

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  • NMR line width of <sup>12</sup>B in Pt detected by β-NMR(共著)

    Hyperfine Interactions   78,439   1993

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  • Quadrupole moment of <sup>41</sup>Sc by use of new nuclear quadrupole resonance detection(共著)

    Hyperfine Interactions   78,191   1993

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  • Precise measurement of the magnetic moment of doubly closed shell-1 nucleon nucleus <sup>15</sup>O(I<sup>π</sup>=1/2-, T<sub>1/2</sub>=122sec)(共著)

    Hyperfine Interactions   78,105   1993

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  • Hyperfine interactions of <sup>12</sup>B in BN(hexagonal)(共著)

    Hyperfine Interactions   78,185   1993

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  • Production of unstable nuclei far from the stability line : its scope and limitations(共著)

    Hyperfine Interactions   80,1219   1993

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  • New nuclear quadrupole resonance technique in β-NMR(共著)

    Hyperfine Interactions   80,1315   1993

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  • Magnetic moment of <sup>23</sup>Mg(共著)

    Hyperfine Interactions   78,117   1993

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  • Electric field gradient in Mg and Zn detected by β-emitters, <sup>8</sup>Li and <sup>12</sup>B(共著)

    Hyperfine Interactions   80,1051   1993

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  • New nuclear quadrupole resonance technique in β-NMR(共著)

    Hyperfine Interactions   80,1315   1993

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  • Electric field gradient in Mg and Zn detected by β-emitters, <sup>8</sup>Li and <sup>12</sup>B(共著)

    Hyperfine Interactions   80,1051   1993

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  • Production of unstable nuclei far from the stability line : its scope and limitations(共著)

    Hyperfine Interactions   80,1219   1993

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  • PRECISE MEASUREMENT OF THE MAGNETIC-MOMENT OF F-17(I(PI)=5/2(+), T(1/2)=64.5 S) AND ITS HYPERFINE INTERACTIONS IN IONIC-CRYSTALS

    T MINAMISONO, T OHTSUBO, Y NAKAYAMA, T ARAKI, K MASHITANI, K MATSUDA, E TAKAHASHI, M TANIGAKI, Y SOMEDA, M TANAKA, A KITAGAWA, M FUKUDA, K MATSUTA, Y NOJIRI

    HYPERFINE INTERACTIONS   73 ( 3-4 )   347 - 356   1992

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    Language:English   Publisher:SPRINGER  

    Hyperfine interactions of beta-emitting F-17 implanted in single crystals of NaF and CaF2 were studied. The nuclear magnetic moment of the I(pi) = 5/2+ state was determined with an improved precision to be \mu(F-17; I(pi) = 5/2+, T1/2 = 64.5 s\ = 4.72130 +/- 0.00025 nm. Isoscalar magnetic moments of die doubly closed shell +/- 1 nucleon nuclei around mass number 16 were derived and the effective nucleon mass in the nucleus was discussed.

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  • Observation of spin polarization of projectile fragments from 106 AMeV <sup>40</sup>Ca+Au collisions(共著)

    Physics Letters B   281,214   1992

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  • Proton halo of <sup>8</sup>B disclosed by its giant quadrupole moment(共著)

    Physical Review Letters   69,2058   1992

  • Proton Halo of <sup>8</sup>B Disclosed by Its Giant Quadrupole Moment(共著)

    Physical Review Letters   69,2058   1992

  • Precise measurement of the magnetic moment of <sup>17</sup>F(I<sup>π</sup>=5/2+, T<sub>1/2</sub>=64.5sec) and its hyperfine interactions in ionic crystals(共著)

    Hyperfine Interactions   73,347   1992

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  • A fragment separator at LBL for the beta-NMR experiment(共著)

    Nuclear Instruments and methods in Physics Research B   70,304   1992

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  • A fragment separator at LBL for the beta-NMR experiment(共著)

    Nuclear Instruments and methods in Physics Research B   70,304   1992

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  • Observation of spin polarization of projectile fragments from 106 AMeV <sup>40</sup>Ca+Au collisions(共著)

    Physics Letters B   281,214   1992

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  • magnetic moments of the doubly closed shell±1 nucleon nuclei and on-line nuclear polarization (共著)

    Hyperfine Interactions   59, 31   1990

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  • Precision measurement of the magnetic moment of <sup>41</sup>Sc(I<sup>π</sup>=7/2<sup>-</sup>, T<sub>1/2</sub>=0.59s) and isoscalar g-factors of orbital and spin angular moment. (共著)

    Nuclear Physics A   516,365   1990

  • Quadrupole moment of the doubly closed shell +1 nucleon nucleus <sup>41</sup>Sc(I<sup>π</sup>=7/2-) (共著)

    Hyperfine Interactions   59, 153   1990

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  • magnetic moments of the doubly closed shell±1 nucleon nuclei and on-line nuclear polarization (共著)

    Hyperfine Interactions   59, 31   1990

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  • NMR on beta-emitting <sup>43</sup>Ti produced through projectile fragmentation relativistic heavy-ion collisions(共著)

    Hyperfine Interactions   61, 1387   1990

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  • Electro Magnetic moment of beta-emitting <sup>41</sup>Sc(I<sup>π</sup>=7/2-) and Knight shift in Pt metal (共著)

    Hyperfine Interactions   59, 149   1990

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  • Precision measurement of the magnetic moment of <sup>41</sup>Sc(I<sup>π</sup>=7/2-, T<sub>1/2</sub>=0.59s) and isoscalar g-factors of orbital and spin angular momenta(共著)

    Nuclear Physics A   516,365   1990

  • Quadrupole moment of the doubly closed shell +1 nucleon nucleus <sup>41</sup>Sc(I<sup>π</sup>=7/2-) (共著)

    Hyperfine Interactions   59, 153   1990

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  • NMR on beta-emitting <sup>43</sup>Ti produced through projectile fragmentation relativistic heavy-ion collisions(共著)

    Hyperfine Interactions   61, 1387   1990

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  • Electro Magnetic moment of beta-emitting <sup>41</sup>Sc(I<sup>π</sup>=7/2-) and Knight shift in Pt metal (共著)

    Hyperfine Interactions   59, 149   1990

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Research Projects

  • 重イオン蓄積リングを用いた不安定核の研究

    2000

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    Grant type:Competitive

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  • Study of unstuble nuclei with heavy ion storuge ring

    2000

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    Grant type:Competitive

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  • 不安定核ビームを用いた核構造研究

    1999

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    Grant type:Competitive

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  • Nuclear structure study with unstabe nuclear been

    1999

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    Grant type:Competitive

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  • 物質中における超微細構造相互作用の研究

    1988

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    Grant type:Competitive

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  • 不安定核の電磁気モーメントの研究

    1988

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    Grant type:Competitive

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  • Study on electromagnetic moments of Unstable nuclei

    1988

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    Grant type:Competitive

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  • Study on the hyperfine interactions in solid

    1988

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    Grant type:Competitive

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Teaching Experience

  • 実験核物理学概論

    2024
    Institution name:新潟大学

  • 電磁気学特論

    2023
    Institution name:新潟大学

  • 原子力・放射線防護学入門

    2023
    Institution name:新潟大学

  • 原子力・放射線物理学入門

    2023
    Institution name:新潟大学

  • 原子力規制学総論

    2023
    Institution name:新潟大学

  • 原子力・放射線関連法規入門

    2023
    Institution name:新潟大学

  • 放射線計測実習

    2023
    Institution name:新潟大学

  • 量子研究の最前線

    2023
    Institution name:新潟大学

  • 原子力規制キャリア教育

    2023
    Institution name:新潟大学

  • 理学基礎演習

    2022
    Institution name:新潟大学

  • 原子核構造特論I

    2022
    Institution name:新潟大学

  • 放射線防護学特論

    2022
    Institution name:新潟大学

  • 放射線物理学特論

    2022
    Institution name:新潟大学

  • 理学スタディ・スキルズ

    2022
    Institution name:新潟大学

  • 物理学特論VI

    2022
    Institution name:新潟大学

  • 原子核物理特論I

    2022
    Institution name:新潟大学

  • 物理学基礎CII

    2021
    Institution name:新潟大学

  • エレクトロニクスA

    2021
    Institution name:新潟大学

  • 放射線計測学特論

    2021
    Institution name:新潟大学

  • エレクトロニクスB

    2021
    Institution name:新潟大学

  • 放射線関連法規

    2021
    Institution name:新潟大学

  • 物理学概論

    2021
    Institution name:新潟大学

  • 数理物質科学の最前線

    2021
    Institution name:新潟大学

  • 原子核構造特論II

    2021
    Institution name:新潟大学

  • 核物性学概論

    2021
    Institution name:新潟大学

  • 自然科学基礎実験

    2021
    Institution name:新潟大学

  • 日本事情自然系A

    2021
    Institution name:新潟大学

  • 物理学実験C

    2020
    Institution name:新潟大学

  • 物理学実験B

    2020
    Institution name:新潟大学

  • 物理学実験A

    2020
    Institution name:新潟大学

  • 原子核物理学

    2020
    Institution name:新潟大学

  • 現代物理学セミナーB

    2020
    Institution name:新潟大学

  • 現代物理学セミナーA

    2020
    Institution name:新潟大学

  • 医学物理学総論

    2020
    Institution name:新潟大学

  • 放射線物理学特論

    2020
    -
    2022
    Institution name:新潟大学

  • 放射線防護学特論

    2020
    -
    2022
    Institution name:新潟大学

  • 物理学特論VI

    2020
    -
    2022
    Institution name:新潟大学

  • 物理学実験D

    2020
    -
    2022
    Institution name:新潟大学

  • 物理学基礎実習a

    2020
    Institution name:新潟大学

  • 物理学基礎実習b

    2020
    Institution name:新潟大学

  • 課題研究C

    2020
    Institution name:新潟大学

  • 課題研究D

    2020
    Institution name:新潟大学

  • 課題研究B

    2019
    -
    2020
    Institution name:新潟大学

  • 課題研究A

    2019
    -
    2020
    Institution name:新潟大学

  • 理学スタディ・スキルズ

    2018
    -
    2022
    Institution name:新潟大学

  • 専門力アクティブ・ラーニング

    2018
    -
    2021
    Institution name:新潟大学

  • 物理学基礎C3

    2017
    -
    2020
    Institution name:新潟大学

  • 物理学基礎C4

    2017
    -
    2020
    Institution name:新潟大学

  • ミュオン物質物理学特論

    2017
    Institution name:新潟大学

  • 原子核物理学I

    2017
    Institution name:新潟大学

  • ミュオン物質物理学概論

    2016
    -
    2022
    Institution name:新潟大学

  • 物理学への招待A

    2014
    Institution name:新潟大学

  • 課題探索特講

    2014
    Institution name:新潟大学

  • 医学物理学入門

    2013
    Institution name:新潟大学

  • 日本事情自然系A

    2013
    -
    2021
    Institution name:新潟大学

  • 物理学概論

    2013
    -
    2021
    Institution name:新潟大学

  • 安全教育

    2013
    -
    2017
    Institution name:新潟大学

  • 医学物理学特論

    2012
    Institution name:新潟大学

  • 計測学

    2012
    -
    2018
    Institution name:新潟大学

  • 数理物質科学特定研究Ⅰ(物理学)

    2012
    -
    2015
    Institution name:新潟大学

  • コラボレーション演習

    2012
    -
    2015
    Institution name:新潟大学

  • 数理物質科学演習Ⅰ(物理学)

    2012
    -
    2015
    Institution name:新潟大学

  • 数理物質科学特定研究ⅡA(物理学)

    2012
    -
    2014
    Institution name:新潟大学

  • 数理物質科学特定研究ⅡB(物理学)

    2012
    -
    2014
    Institution name:新潟大学

  • 数理物質科学演習Ⅱ(物理学)

    2012
    -
    2014
    Institution name:新潟大学

  • 原子核物理学特論

    2012
    Institution name:新潟大学

  • 核物性学概論

    2011
    -
    2021
    Institution name:新潟大学

  • 原子核構造特論Ⅱ

    2011
    -
    2017
    Institution name:新潟大学

  • 物理学実験

    2010
    -
    2016
    Institution name:新潟大学

  • 物理学最前線入門

    2010
    Institution name:新潟大学

  • 原子核物理特論Ⅰ

    2008
    -
    2020
    Institution name:新潟大学

  • 原子核物理学II

    2008
    -
    2018
    Institution name:新潟大学

  • 原子核構造特論Ⅰ

    2008
    -
    2016
    Institution name:新潟大学

  • 原子核物理特論I

    2007
    -
    2022
    Institution name:新潟大学

  • 原子核構造特論I

    2007
    -
    2022
    Institution name:新潟大学

  • 物理学実験a

    2007
    -
    2016
    Institution name:新潟大学

  • 物理学実験b

    2007
    -
    2016
    Institution name:新潟大学

  • 初等物理学実験

    2007
    -
    2012
    Institution name:新潟大学

  • 物理学基礎実験

    2007
    -
    2012
    Institution name:新潟大学

  • 計算物理学演習

    2007
    -
    2011
    Institution name:新潟大学

  • 現代物理学への招待(物理学学習法)

    2007
    -
    2009
    Institution name:新潟大学

▶ display all