Microscopic structure of the Gamow-Teller resonance in Cu-58

The 2osPb(3He,t)20sBi reaction has been studied with the RCNP ring cyclotron at E(3He) = 450 MeV using the magnetic spectrometer Grand Raiden at 0 = 0”. The Gamow-Teller resonance is strongly excited at this bombarding energy. Its microscopic structure has been investigated by measuring the direct proton decay to the neutron-hole states in ‘07Pb. The branching ratio for proton emission of a few % is much smaller than that for the decay of the isobaric analog state. The total width of the Gamow-Teller resonance as well as its total and partial escape widths have been determined. Several recent theoretical estimates for the escape width differ from the measured values by factors of - 2.5.

[1]  M. Nakano,et al.  Isobaric analog states observed in the 58Ni(p,d)57Ni reaction with 65 MeV polarized protons , 2000 .

[2]  D. Roberts,et al.  Search for isovector giant monopole resonances via the ^{124}Sn (^{3}He,tn) reaction , 2000 .

[3]  A. Tamii,et al.  Magnetic spectrometer Grand Raiden , 1999 .

[4]  M. R. Bhat Nuclear Data Sheets for A ;eq 58 , 1997 .

[5]  M. Fujiwara,et al.  DIRECT PROTON DECAY FROM THE GAMOW-TELLER RESONANCE IN BI-208 , 1995 .

[6]  Masayoshi Tanaka,et al.  (3He,t) Charge-Exchange Reactions at E(3He) = 450 MeV, θ = 0° , 1994 .

[7]  Huo Junde Nuclear data sheets update for A = 56 , 1992 .

[8]  C. Gaarde Spin Excitations in Nuclei , 1990 .

[9]  A. Hees,et al.  Electroexcitation of 58ni: A sutdy of the fragmentation of the magnetic dipole strength , 1987 .

[10]  A. Arima Nuclear magnetic properties and gamow-teller transitions , 1984 .

[11]  T. P. Welch,et al.  Excitation of giant spin-isospin multipole vibrations in 54,56 Fe and 58,60 Ni , 1983 .

[12]  M. Fujiwara,et al.  M1 states in 58Ni observed by proton inelastic scattering at 65 MeV , 1983 .

[13]  T. P. Welch,et al.  Excitation of Gamow-Teller resonances in A=58 nuclei , 1982 .

[14]  P. Kitching,et al.  Systematics of the excitation of M1 resonances in medium heavy nuclei by 200 MeV proton inelastic scattering , 1982 .

[15]  P. Kitching,et al.  M1 strength in zirconium isotopes by proton inelastic scattering , 1982 .

[16]  R. Stock,et al.  Ground state dipole transitions in 58Ni , 1981 .

[17]  C. Djalali,et al.  Observation of M1 Strength by the Inelastic Scattering of 200-MeV Protons , 1981 .

[18]  M. Fujiwara,et al.  Systematic observation of fine structure of the hole-state analogues in Ni isotopes , 1979 .

[19]  F. Pühlhofer On the interpretation of evaporation residue mass distributions in heavy-ion induced fusion reactions , 1977 .

[20]  X. K. Maruyama,et al.  Electroexcitation of the T/sub 0/ + 1 giant M1 resonance in /sup 58/,/sup 60/Ni , 1976 .

[21]  H. Vonach,et al.  Level density parameters for the back-shifted fermi gas model in the mass range 40 < A < 250 , 1973 .

[22]  P. Hinrichsen,et al.  Particle-γ-Ray Angular-Correlation Study of 57 Ni in the Reaction 58 Ni( 3 He,αγ) 57 Ni , 1969 .

[23]  E. Gadioli,et al.  Level Density of Light Nuclei , 1968 .