“…These phenomenological models with simplified assumptions are usually more computationally accessible but are limited to excitation energies above 5 MeV. Microscopic models, such as Hartree-Fock-Bardeen-Cooper-Schrieffer (HF-BCS) [9], Gogny-Hartree-Fock-Bogoliubov (Gogny-HFB) [10], and Skyrme-Hartree-Fock-Bogoliubov (Skyrme-HFB) [11], and density functional theory combinatorial models [12,13], the Monte Carlo shell model [14], quasi-particle random phase approximation (QRPA) [15], and core-quasi particle coupling (CQC) model [16], have attempted to describe the NLD from more fundamental particle interactions with excitation energies ranging from 0 to 20 MeV. Thus, a high efficiency and unified predictive model is urgently required for the application of NLD.…”