摘要
Nuclear magnetic moment is an important physical variable and serves as a useful tool for the stringent test of nuclear models. For the past decades, the covariant density functional theory and its extension have been proved to be successful in describing the nuclear ground-states and excited states properties. However, a long-standing problem is its failure to predict magnetic moments. This article reviews the recent progress in the description of the nuclear magnetic moments within the covariant density functional theory. In particular, the magnetic moments of spherical odd-A nuclei with doubly closed shell core plus or minus one nucleon and deformed odd-A nuclei.
Nuclear magnetic moment is an important physical variable and serves as a useful tool for the stringent test of nuclear models. For the past decades, the covariant density functional theory and its extension have been proved to be successful in describing the nuclear ground-states and excited states properties. However, a long-standing problem is its failure to predict magnetic moments. This article reviews the recent progress in the description of the nuclear magnetic moments within the covariant density functional theory. In particular, the magnetic moments of spherical odd-A nuclei with doubly closed shell core plus or minus one nucleon and deformed odd-A nuclei.
作者
Jian Li
J.Meng
李剑;孟杰(College of Physics, Jilin University, Changchun 130012,China;Department of Physics, Western Michigan University, Kalamazoo, China MI 49008, USA;State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing 100871, China;Yukawa Institute for Theoretical Physics, Kyoto University, Kyoto 606-8502, Japan;Department of Physics, University of Stellenbosch, Stellenbosch, South Africa)
