Level density of odd-A nuclei at saddle point  

作　　者：Wei Zhang Wei Gao Gui-Tao Zhang Zhi-Yuan Li 

机构地区：[1]School of Physics and Microelectronics,Zhengzhou University,Zhengzhou 450001,China

出　　处：《Nuclear Science and Techniques》2023年第8期164-173,共10页核技术（英文）

基　　金：supported by the China Institute of Atomic Energy(No.401Y-FW-GKXJ-21-1496);the Natural Science Foundation of Henan Province(No.202300410480 and 202300410479);the Open Project of Guangxi Key Laboratory of Nuclear Physics and Nuclear Technology(No.NLK2021-01);the National Natural Science Foundation of China(No.U2032141).

摘　　要：Based on the covariant density functional theory,by employing the core–quasiparticle coupling(CQC)model,the nuclear level density of odd-A nuclei at the saddle point is achieved.The total level density is calculated via the convolution of the intrinsic level density and the collective level density.The intrinsic level densities are obtained in the finite-temperature covariant density functional theory,which takes into account the nuclear deformation and pairing self-consistently.For saddle points on the free energy surface in the(β_(2),γ)plane,the entropy and the associated intrinsic level density are compared with those of the global minima.By introducing a quasiparticle to the two neighboring even–even core nuclei,whose properties are determined by the five-dimensional collective Hamiltonian model,the collective levels of the odd-A nuclei are obtained via the CQC model.The total level densities of the^(234-240)U agree well with the available experimental data and Hilaire’s result.Furthermore,the ratio of the total level densities at the saddle points to those at the global minima and the ratio of the total level densities to the intrinsic level densities are discussed separately.

关 键 词：Level density Covariant density functional theory Core–quasiparticle coupling model Saddle point 

分 类 号：O571[理学—粒子物理与原子核物理]