High-resolution study of Gamow-Teller transitions in the 47Ti(3He,t)47V reaction
Tarih
2013Yazar
Rubio, B.
Estevez-Aguado, E.
Guess, C. J.
Gulyas, J.
Hatanaka, K.
Hirota, K.
Honma, M.
Ishikawa, D.
Krasznahorkay, A.
Matsubara, H.
Meharchand, R.
Molina, F.
Okamura, H.
Ong, H. J.
Otsuka, T.
Perdikakis, G.
Fujita, H.
Scholl, C.
Shimbara, Y.
Suzuki, T.
Tamii, A.
Thies, J. H.
Zegers, R. G. T.
Zenihiro, J.
Ganioglu, Ela
Susoy, Gülfem
Fujita, Y.
Adachi, T.
Algora, A.
Csatlos, M.
Deaven, J. M.
Üst veri
Tüm öğe kaydını gösterÖzet
Given the importance of Gamow-Teller (GT) transitions in nuclear structure and astrophysical nuclear processes, we have studied T-z = +3/2 -> +1/2, GT transitions starting from the Ti-47 nucleus in the (He-3, t) charge-exchange reaction at 0 degrees and at an intermediate incident energy of 140 MeV/nucleon. The experiments were carried out at the Research Center for Nuclear Physics (RCNP), Osaka, using the high-resolution facility with a high-dispersion beam line and the Grand-Raiden spectrometer. With an energy resolution of 20 keV, individual GT transitions were observed and GT strength was derived for each state populated up to an excitation energy (E-x) of 12.5 MeV. The GT strength was widely distributed from low excitation energy up to 12.5 MeV, where we had to stop the analysis because of the high level density. The distribution of the GT strengths was compared with the results of shell model calculations using the GXPF1 interaction. The calculations could reproduce the experimental GT distributions well. The GT transitions from the ground state of Ti-47 and the M1 transitions from the isobaric analog state in V-47 to the same low-lying states in V-47 are analogous. It was found that the ratios of GT transition strengths to the ground state, the 0.088-MeV state, and the 0.146-MeV state are similar to the ratios of the strengths of the analogous M1 transitions from the isobaric analog state (IAS) to these states. The measured distribution of the GT strengths was also compared with those starting from the T-z = +3/2 nucleus K-41 to the T-z = +1/2 nucleus Ca-41. DOI: 10.1103/PhysRevC.87.014321
Bağlantı
http://hdl.handle.net/20.500.12627/50099https://doi.org/10.1103/physrevc.87.014321
https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84872707049&origin=inward
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