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| 1 | Nuclear Structure and Magnetic Moment of the Unstable 12B-12N Mirror Pair显示文摘 | 郑永男 周冬梅 袁大庆 左翼 范平 M. Mihara K. Matsuta M. Fukuda T. Minamisono T. Suzuki 徐勇军 朱佳政 王志强 骆海龙 张锡珍 朱升云 | 2010 | Chinese Physics Letters2010，27，2： | 2 |
| 2 | Fetal germinal matrix and intraventricular haemorrhage diagnosed by MRI显示文摘 | K. Fukui T. Morioka S. Nishio F. Mihara H. Nakayama K. Tsukimori M. Fukui | 2001 | Neuroradiology2001，，1： | 1 |
| 3 | Magnetic properties of commercially produced Fe-6.5wt% Si sheet显示文摘 | M. Abe Y. Takada T. Murakami Y. Tanaka Y. Mihara | 1989 | Journal of Materials Engineering1989，，1： | 1 |
| 4 | Experimental study of critical heat flux in open two-phase thermosyphon显示文摘 | M. Monde S. Mihara Y. Mitsutake | 1996 | Heat and Mass Transfer1996，，6： | 1 |
| 5 | Study on reaction kinetics and selective precipitation of Cu, Zn, Ni and Sn with H 2 S in single-metal and multi-metal systems显示文摘 | H. Tokuda D. Kuchar N. Mihara M. Kubota H. Matsuda T. Fukuta | 2008 | Chemosphere2008，，9： | 1 |
| 6 | Precise measurement of magnetic moment of short-lived β-emitting nuclei ^(12)B (I~π=1^+,T_(1/2)=20.18 ms)显示文摘The spin polarized -emitting nuclei 12B (I p = 1+, T1/2 = 20.18 ms) were produced by the nuclear reaction 11B(d, p) 12B and by the selection technique of the incident deuteron energy and the 12B recoil angle following the nuclear reaction. The nuclear magnetic moment of the short-lived nuclei 12B was measured by ?NMR with the -NMR and -NQR setup established for the first time in China. The nuclear magnetic moment of 12B was determined to be = 0.99993 0.00048 nm or g = 0.99993 0.00048 after the precise correction of the Knight shift. | M. Mihara M. Fukuda K. Matsuta T. Minamisono | 2004 | Science China(Physics,Mechanics & Astronomy)2004，47，5： | 1 |
| 7 | IL ‐6 receptor antagonist as adjunctive therapy with clotting factor replacement to protect against bleeding‐induced arthropathy in hemophilia显示文摘 | N. Narkbunnam J. Sun G. Hu F.‐C. Lin T. A. Bateman M. Mihara P. E. Monahan | 2013 | J Thromb Haemost2013，，5： | 1 |
| 8 | Dependence of Quasi-Particle Alignment on Proton Number in N=44 Isotones ^(82)Sr,^(83)Y,^(84)Zr and ^(85)Nb显示文摘The g-factors of Ground Rotational Band states of N=44 isotones 82Sr, 83Y, 84Zr and 85Nb have been measured by the transient-magnetic-field ion implantation perturbed angular distribution (TMF-IMPAD) method. The measured g-factors of 82Sr increase with the increase of spin I, indicating a proton alignment only. Positive peaks appear in the variation of g-factors with spin for 83Y and 84Zr at spin 21/2+ and 10+ respectively, indicating a proton alignment followed by a neutron alignment. A negative peak occurs for 85Nb at the spin25/2+ , indicating a neutron alignment followed by a proton alignment. | 范平 袁大庆 郑永男 左翼 周冬梅 张乔丽 吴晓光 李广生 竺礼华 许国基 樊启文 张锡珍 T. MINAMISONO K. MATSUTA M. FUKUDA M. MIHARA 朱升云 | 2012 | Plasma Science and Technology2012，14，5： | 0 |
| 9 | Magnetic Moment Measurement of ^(28)P显示文摘The last proton separation energy of β-emitting nuclide 28P is 0.6 MeV and its last proton occupies the orbit 2s1/2. At present, all of the results showed that there exists proton halo structure in 28P, whether from the measurements of cross section or from the theoretical study. No magnetic moment or | ZHOU Dong-mei ZHENG Yong-nan YUAN Da-qing ZUO Yi LIU Meng FAN Ping M. Mihara M. Fukuda K. Matsuta T. Minamisono T. Nagatomo S. Momota A. Kitagawa T. Izumikawa ZHU Sheng-yun | 2006 | Annual Report of China Institute of Atomic Energy2006，，1： | 0 |
| 10 | Nuclear structure of proton-rich unstable nucleus ^(28)P studied by g-factor measurement显示文摘Nuclear structure of proton-rich unstable nucleus 28P has been studied by measuring its g-factor for the first time. The g-factor of 28P (Iπ =3+, T1/2=270.3 ms) was measured by means of β-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 β-ray transition probability, the orbital angular momenta and intrinsic spins of protons and neutrons have been determined as lp =0.43(29), ln =1.85(29), Sp)=0.28(4), and Sn =0.44(4). | 郑永男 周冬梅 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 袁大庆 左翼 范平 T. Suzuki 张锡珍 朱升云 | 2009 | Chinese Physics C2009，33，S1： | 0 |
| 11 | β-放射性核^(12)N的磁矩测量显示文摘 | 郑永男 周冬梅 杜恩鹏 袁大庆 左翼 王志强 骆海龙 M. Mihara M Fukuda K. Matsuta T. Minamisono 朱升云 | 2003 | 中国原子能科学研究院年报2003，，1： | 0 |
| 12 | β-NMR和β-NQR的数据获取系统显示文摘 | 袁大庆 周冬梅 郑永男 杜恩鹏 左翼 王志强 骆海龙 M. Mihara M Fukuda K. Matsuta T. Minamisono 朱升云 | 2003 | 中国原子能科学研究院年报2003，，1： | 0 |
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