“…Earlier calculations of charged-current neutrino-nucleus scattering cross sections have been carried out for various nuclei in the nuclear shell model [11][12][13][14][15][16], proton-neutron quasiparticle random-phase approximation (pnQRPA) with realistic effective interactions [17][18][19][20][21], pnQRPA based on Skyrme forces [12,[22][23][24], pnQRPA with neutron-proton pairing [25][26][27], a consistent relativistic mean-field approach [28], a hybrid model combining shell model for the allowed transitions and pnQRPA for forbidden transitions [29][30][31], and the microscopic quasiparticle-phonon model (MQPM) [21,32]. In the present work we compute cross sections of neutrinos and antineutrinos scattering off 128 Xe, 129 Xe, 130 Xe, 131 Xe, 132 Xe, 134 Xe, and 136 Xe via charged-current processes in the microscopic nuclear frameworks of pnQRPA for the even-mass nuclei and MQPM for the odd-mass nuclei.…”