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排序方式: 共有95条查询结果,搜索用时 187 毫秒
31.
H. Bhang S. Ajimura K. Aoki A. Banu T. Fukuda O. Hashimoto J. I. Hwang S. Kameoka B. H. Kang E. H. Kim J. H. Kim M. Kim T. Maruta Y. Miura Y. Miyake T. Nagae M. Nakamura S. N. Nakamura H. Noumi S. Okada Y. Okayasu H. Outa H. Park P. K. Saha Y. Sato M. Sekimoto S. Shin T. Takahashi H. Tamura K. Tanida A. Toyota K. Tsukada T. Watanabe H. J. Yim 《The European Physical Journal A - Hadrons and Nuclei》2007,33(3):259-263
Recent exclusive coincidence measurements of non-mesonic weak decays (NMWD) reported for the ratio of the partial decay width
of neutron-induced-to-proton-induced NMWD, Γn/Γp , values of 0.45±0.11±0.03 and 0.51±0.13±0.04 for 5lam and 12
Λ
C , respectively. These observations agree well with the improved theoretical Γn/Γp ratios which are in the range of 0.3-0.7. It appears that the long-standing discrepancy between the experimental and theoretical
values of Γn/Γp has finally been solved. However, when compared to the results of intra-nuclear cascade (INC) calculations, the observed
numbers of both single nucleons and coincident nucleon pairs are strongly quenched. The quenching of the proton yield observed
previously has been interpreted as an increase of the Γn/Γp ratio. On the other hand, significant contributions from the two-nucleon-induced three-body process ΛNN → nNN are predicted. Indeed, the angular correlation of the emitted nucleon pairs in the NMWD of 12
Λ
C showed not only decay events in back-to-back kinematics, but also events with non-back-to-back kinematics. In this paper
we show that the difficulties to extract the correct Γn/Γp ratio from the proton spectra is related to the three-body weak-interaction process which strongly quenches the nucleon yields. 相似文献
32.
Y. Ichikawa H. C. Bhang S. Bufalino H. Ekawa P. Evtoukhovitch A. Feliciello H. Fujioka S. Hasegawa S. Hayakawa R. Honda K. Hosomi K. Imai S. Ishimoto C. W. Joo S. Kanatsuki R. Kiuchi T. Koike H. Kumawat Y. Matsumoto K. Miwa M. Moritsu T. Nagae M. Naruki M. Niiyama Y. Nozawa R. Ota A. Sakaguchi H. Sako V. Samoilov S. Sato K. Shirotori H. Sugimura S. Suzuki T. Takahashi T. N. Takahashi H. Tamura T. Tanaka K. Tanida A. O. Tokiyasu Z. Tsamalaidze B. J. Roy M. Ukai T. O. Yamamoto S. B. Yang 《Few-Body Systems》2013,54(7-10):1191-1194
In the J-PARC E27 experiment, we search for a K ? pp bound state via the d(π +, K +) reaction at 1.7 GeV/c at the K1.8 beam line. The binding energy and decay width of the K ? pp bound state can be obtained in the missing mass measurement with a good energy resolution of 2 MeV/c 2. A range counter array (RCA) was constructed to detect the two high-momentum protons from the K ? pp decay and to reduce the background such as quasi-free hyperon production. Recently, we have carried out a pilot run in June, 2012. The d(π +, K +) missing-mass spectrum has been obtained for the first time. In this report, an overview of the E27 experiment and a preliminary result on this pilot run are presented. 相似文献
33.
Ajimura S Ikeda K Ishikawa M Kishimoto T Okusu A Shinkai N Tanaka Y Ejiri H Nakano T Manabe K Nagae T Noumi H Sekimoto M Shibata T Hashimoto O Maeda K Takahashi T Hasegawa T Bhang H Kim YD Park H Youn M 《Physical review letters》2000,84(18):4052-4055
We have measured the asymmetric emission of protons from the nonmesonic decay of polarized (5)(Lambda)He produced by the (pi(+), K+) reaction. (5)(Lambda)He is an s-shell hypernucleus and its polarization is due to the Lambda. One expects to obtain direct information on the elementary weak Lambda-->p-->np process. The asymmetry parameter has been determined to be 0.24+/-0.22. The implication of the result is discussed. 相似文献
34.
Mixed-valent imido-bridged dinuclear titanium complexes, [Cp(2)Co][{(C(5)R(5))TiCl}(2)(μ-NAr)(2)] (R = H, Me; Ar = 3,5-(CF(3))(2)C(6)H(3)), were prepared by one-electron reduction of the corresponding [(C(5)R(5))TiCl](2)(μ-NAr)(2). One unpaired electron is delocalized in the central Ti(μ-NR)(2)Ti core as the first example of a fully delocalized mixed-valent imido-bridged [Ti(2)](7+) species. 相似文献
35.
Suguru Nagae Yasuo Suda Yoshiaki Inaki Kiichi Takemoto 《Journal of polymer science. Part A, Polymer chemistry》1989,27(8):2593-2609
Poly-L -lysine (PLL) derivatives containing pendant nucleic acid base, such as thymine or adenine, were bonded successfully to 3-aminopropylsilanized silica (APS-silica) and silica gel. These resins were found to be useful as the column of high performance liquid chromatography (HPLC) for the selective separation of oligoethyleneimine derivatives having pendant thymine or adenine bases. 相似文献
36.
Michitaka Kuici Hiroyoshi Nagae Richard J. Cogdell Keizo Shimada Yasushi Koyama 《Photochemistry and photobiology》1994,59(1):116-124
Abstract –The 1Ag?→1Bu+ electronic absorption band and the vibronically coupled, C=C stretching Raman lines in the 1Ag? and 21Ag? states were recorded for spheroidene free in nonpolar and polar solvents as well as for spheroidene bound to the LH1 and LH2 complexes of Rhodobacter sphaeroides 2.4.1. The 1Bu+ energy exhibited a linear dependence on R(n) = (n2 - 1)/(n2+ 2) in both nonpolar and polar solvents; the line for polar solvents had a gentler slope and crossed the line for nonpolar solvents at R(n) = 0.3. The above characteristic of polar solvents was ascribed to the electric field generated by fluctuation of the solvent permanent dipoles; it stabilizes the 1Bu+ energy and reduces the polarizability of the solvent. The vibronically coupled, C=C stretching frequencies in the 1Ag? and 21Ag? states [ν(Ag) and [ν(2Ag)] also showed similar dependence on R(n), which is explained in terms of vibronic coupling among the 1Ag?, 21Ag? and 31Ag? states. The environment of spheroidene in the LH2 and LH1 complexes was assessed on the basis of the 1Bu+ energy and the ν(Ag) and [ν(2Ag) frequencies: Spheroidene in the LH2 complex is located in an environment with high polarizability, while spheroidene in the LH1 complex is located in an environment with lower polarizability. 相似文献
37.
38.
T.Nagae 《中国物理C(英文版)》2010,34(9)
We have held an inauguration ceremony of the Japan Proton Accelerator Research Complex (J-PARC) on July 6, 2009, celebrating the completion of its construction. Now, the beam commissioning of the 50 GeV main proton synchrotron is in progress to improve the beam intensity and quality. A lot of important experimental programs in Nuclear Physics are waiting for the beam. In this report, I introduce some examples. 相似文献
39.
Saha PK Fukuda T Imoto W Ahn JK Ajimura S Aoki K Bhang HC Fujioka H Hotchi H Hwang JI Itabashi T Kang BH Kim HD Kim MJ Kishimoto T Krutenkova A Maruta T Miura Y Miwa K Nagae T Noumi H Outa H Ohtaki T Sakaguchi A Sato Y Sekimoto M Shimizu Y Tamura H Tanida K Toyoda A Ukai M Yim HJ 《Physical review letters》2005,94(5):052502
In order to produce a neutron-rich Lambda hypernucleus for the first time, we carried out an experiment by utilizing the (pi-,K+) double charge-exchange reaction on a 10B target. We observed the production of a 10LambdaLi hypernucleus. The cross section for the Lambda bound region was found to be 11.3+/-1.9 nb/sr with the 1.2 GeV/c incident momentum, which is compared with the 10LambdaB hypernucleus production cross section, 7.8+/-0.3 microb/sr, in the (pi+,K+) reaction with a 1.05 GeV/c incident momentum beam. 相似文献
40.
Noumi H Saha PK Abe D Ajimura S Aoki K Bhang HC Endo T Fujii Y Fukuda T Guo HC Imai K Hashimoto O Hotchi H Kim EH Kim JH Kishimoto T Krutenkova A Maeda K Nagae T Nakamura M Outa H Sekimoto M Saito T Sakaguchi A Sato Y Sawafta R Shimizu Y Takahashi T Tang L Tamura H Tanida K Watanabe T Xia HH Zhou SH Zhu LH Zhu XF 《Physical review letters》2002,89(7):072301
We have studied the (pi(-),K+) reaction on a silicon target to investigate the sigma-nucleus potential. The inclusive spectrum was measured at a beam momentum of 1.2 GeV/c with an energy resolution of 3.3 MeV (FWHM) by employing the superconducting kaon spectrometer system. The spectrum was compared with theoretical calculations within the framework of the distorted-wave impulse approximation, which demonstrates that a strongly repulsive sigma-nucleus potential with a nonzero size of the imaginary part reproduces the observed spectrum. 相似文献