Dataset referencing 2018GO15
S.Goriely, S.Hilaire, S.Peru, K.Sieja
Gogny-HFB+QRPA dipole strength function and its application to radiative nucleon capture cross section
NUCLEAR STRUCTURE 72,74,76Ge, 75As, 76,80,82Se, 90,92,94Zr, 103Rh, 107,109Ag, 115In, 112,114,117,118,119,120,122,124Sn, 127I, 133Cs, 136,138Ba, 141Pr, 142,143,144,145,146,148,150Nd, 144,148,149,150,152,153,154Sm, 153Eu, 156,160Gd, 159Tb, 165Ho, 168Er, 171,174Yb, 175,176Lu, 178,180Hf, 182,184,186W, 186,188,189,190,192Os, 191,193Ir, 194,195,196,198Pt, 44Sc, 44Ti, 134Xe, 50V, 56Fe, 89Y, 92,94,96,98Mo, 106,108Pd, 106,112Cd, 139La, 162,164Dy, 167Er, 180,182Ta, 206,208Pb, 232Th, 232Pa, 237,238,239U, 238Np; calculated E1 and M1 deexcitation strength functions, and compared with experimental GDR and Oslo strengths. A=40-250, Z=20-83; calculated total average radiative widths, and compared with experimental data, ratios of theoretical to experimental MACS at kT=30 keV. Z=8-94, N=10-190; calculated ratio of (n, γ) and (p, γ) MACS at T=109 K obtained using D1M+QRPA+0lim+ and the ones obtained using the generalized Lorentzian (GLO) model for nuclei between the neutron and proton driplines. Axially symmetric deformed quasiparticle random-phase approximation with finite-range D1M Gogny force (Gogny-HFB+QRPA).
NUCLEAR REACTIONS 135Ba(n, γ), E=1 keV-1 MeV; 100Mo(n, γ), E=1 keV-20 MeV; calculated σ(E) with D1M+QRPA E1 and M1 strengths, and compared with experimental data. Cl(p, γ), E=172.5 MeV; calculated ratio of (n, γ) MACS at T=109 K obtained using D1M+QRPA+0lim+ and the ones obtained using the generalized Lorentzian (GLO) model.
doi: 10.1103/PhysRevC.98.014327