Based on the Hugenholtz-Van Hove theorem six basic quantities of the EoS in isospin asymmetric nuclear matter are expressed in terms of the nucleon kinetic energy t(k),the isospin symmetric and asymmetric parts of the...Based on the Hugenholtz-Van Hove theorem six basic quantities of the EoS in isospin asymmetric nuclear matter are expressed in terms of the nucleon kinetic energy t(k),the isospin symmetric and asymmetric parts of the single-nucleon potentials U_(0)(ρ,k)and U_(sym,i)(ρ,k).The six basic quantities include the quadratic symmetry energy E_(sym,2)(ρ),the quartic symmetry energy E_(sym,4)(ρ),their corresponding density slopes L_(2)(ρ)and L_(4)(ρ),and the incompressibility coefficients K_(2)(ρ)and K_(4)(ρ).By using four types of well-known effective nucleon-nucleon interaction models,namely the BGBD,MDI,Skyrme,and Gogny forces,the density-and isospin-dependent properties of these basic quantities are systematically calculated and their values at the saturation density q_(0)are explicitly given.The contributions to these quantities from t(k)U_(0)(ρ,k),and U_(sym,i)(ρ,k)are also analyzed at the norma nuclear density q_(0).It is clearly shown that the first-order asymmetric term U_(sym,1)(ρ,k)(also known as the symmetry potential in the Lane potential)plays a vital role in determining the density dependence of the quadratic symmetry energy E_(sym,2)(ρ).It is also shown that the contributions from the high-order asymmetric parts of the single-nucleon potentials(U_(sym,i)(ρ,k)with i>1)cannot be neglected in the calculations of the other five basic quantities Moreover,by analyzing the properties of asymmetric nuclear matter at the exact saturation densityρ_(sat)(δ),the corresponding quadratic incompressibility coefficient is found to have a simple empirical relation K_(sat,2)=K_(2)(ρ_(0))-4.14L_(2)(ρ_(0))展开更多
Based on the newest experimentally extracted nuclear density distributions for double-magic nucleus208Pb(Tarbert et al. in Phys Rev Lett 112:242502, 2014),the sensitivity of α-decay half-life to nuclear skin thicknes...Based on the newest experimentally extracted nuclear density distributions for double-magic nucleus208Pb(Tarbert et al. in Phys Rev Lett 112:242502, 2014),the sensitivity of α-decay half-life to nuclear skin thickness is explored in the vicinity of the shell closure region around208 Pb, i.e., isotopes of Z ? 82 and isotones of N ? 126.With the two-parameter Fermi(2PF) density distributions and an analytically derived formula, the α-decay half-life is found to be closely related to the magnitude of nuclear skin thickness. For a decays to the Z ? 82 isotopes, the α-decay half-life is found to decrease with the increasing neutron skin thickness, while the opposite behavior is found for a decays to the N ? 126 isotones. Therefore, it could be a possible way to extract the nuclear skin thickness from measured α-decay half-lives.展开更多
In this paper,by considering the electrons in different external environments,including neutral atoms,a metal,and an extremely strong magnetic-field environment,the screened a-decay half-lives of the a emitters with p...In this paper,by considering the electrons in different external environments,including neutral atoms,a metal,and an extremely strong magnetic-field environment,the screened a-decay half-lives of the a emitters with proton number Z = 52–105 are systematically calculated.In the external environment,the decay energy and the interaction potential between a particle and daughter nucleus are both changed due to the electron screening effect and their variations are both very important for the electron screening effect.Besides,the electron screening effect is found to be closely related to the decay energy and its proton number.展开更多
Using bare Argonne V4'(AV4'),V6'(AV6'),and V8'(AV8')nucleon–nucleon(NN)interactions,the nuclear equations of state(EOSs)for neutron matter are calculated with the unitary correlation operator ...Using bare Argonne V4'(AV4'),V6'(AV6'),and V8'(AV8')nucleon–nucleon(NN)interactions,the nuclear equations of state(EOSs)for neutron matter are calculated with the unitary correlation operator and high-momentum pair methods.Neutron matter is described using a finite particle number approach with magic number N=66 under a periodic boundary condition.The central short-range correlation originating from the short-range repulsion in the NN interaction is treated by the unitary correlation operator method(UCOM),and the tensor correlation and spin-orbit effects are described by the two-particle two-hole(2p2h)excitations of nucleon pairs,where the two nucleons with a large relative momentum are regarded as a high-momentum(HM)pair.With increasing 2p2h configurations,the total energy per particle of the neutron matter is well-converged under this UCOM+HM framework.Comparing the results calculated with AV4',AV6',and AV8'NN interactions,we demonstrate the effects of the short-range correlation,tensor correlation,and spin-orbit coupling on the density dependence of the total energy per particle of neutron matter.Moreover,the contribution of each Hamiltonian component to the total energy per particle is discussed.The EOSs of neutron matter calculated within the present UCOM+HM framework agree with the calculations of six microscopic many-body theories,especially the auxiliary field-diffusion Monte Carlo calculations.展开更多
基金supported by the National Natural Science Foundation of China(No.11822503)。
文摘Based on the Hugenholtz-Van Hove theorem six basic quantities of the EoS in isospin asymmetric nuclear matter are expressed in terms of the nucleon kinetic energy t(k),the isospin symmetric and asymmetric parts of the single-nucleon potentials U_(0)(ρ,k)and U_(sym,i)(ρ,k).The six basic quantities include the quadratic symmetry energy E_(sym,2)(ρ),the quartic symmetry energy E_(sym,4)(ρ),their corresponding density slopes L_(2)(ρ)and L_(4)(ρ),and the incompressibility coefficients K_(2)(ρ)and K_(4)(ρ).By using four types of well-known effective nucleon-nucleon interaction models,namely the BGBD,MDI,Skyrme,and Gogny forces,the density-and isospin-dependent properties of these basic quantities are systematically calculated and their values at the saturation density q_(0)are explicitly given.The contributions to these quantities from t(k)U_(0)(ρ,k),and U_(sym,i)(ρ,k)are also analyzed at the norma nuclear density q_(0).It is clearly shown that the first-order asymmetric term U_(sym,1)(ρ,k)(also known as the symmetry potential in the Lane potential)plays a vital role in determining the density dependence of the quadratic symmetry energy E_(sym,2)(ρ).It is also shown that the contributions from the high-order asymmetric parts of the single-nucleon potentials(U_(sym,i)(ρ,k)with i>1)cannot be neglected in the calculations of the other five basic quantities Moreover,by analyzing the properties of asymmetric nuclear matter at the exact saturation densityρ_(sat)(δ),the corresponding quadratic incompressibility coefficient is found to have a simple empirical relation K_(sat,2)=K_(2)(ρ_(0))-4.14L_(2)(ρ_(0))
基金supported by the National Natural Science Foundation of China(Nos.11175085,11235001,11375086,and 11120101005)the 973 Program of China(No.2013CB834400)+1 种基金the Project Funded by the Priority Academic Program Development of Jiangsu Higher Education Institutions(PAPD)the Open Project Program of the State Key Laboratory of Theoretical Physics,Institute of Theoretical Physics,Chinese Academy of Sciences,China(No.Y5KF141CJ1)
文摘Based on the newest experimentally extracted nuclear density distributions for double-magic nucleus208Pb(Tarbert et al. in Phys Rev Lett 112:242502, 2014),the sensitivity of α-decay half-life to nuclear skin thickness is explored in the vicinity of the shell closure region around208 Pb, i.e., isotopes of Z ? 82 and isotones of N ? 126.With the two-parameter Fermi(2PF) density distributions and an analytically derived formula, the α-decay half-life is found to be closely related to the magnitude of nuclear skin thickness. For a decays to the Z ? 82 isotopes, the α-decay half-life is found to decrease with the increasing neutron skin thickness, while the opposite behavior is found for a decays to the N ? 126 isotones. Therefore, it could be a possible way to extract the nuclear skin thickness from measured α-decay half-lives.
基金supported by the National Natural Science Foundation of China(Nos.11175085,11235001,11375086,and 11120101005)by the 973 Program of China(No.2013CB834400)+1 种基金by the Project Funded by the Priority Academic Program Development of Jiangsu Higher Education Institutions(PAPD)by the Open Project Program of the State Key Laboratory of Theoretical Physics,Institute of Theoretical Physics,Chinese Academy of Sciences,China(No.Y5KF141CJ1)
文摘In this paper,by considering the electrons in different external environments,including neutral atoms,a metal,and an extremely strong magnetic-field environment,the screened a-decay half-lives of the a emitters with proton number Z = 52–105 are systematically calculated.In the external environment,the decay energy and the interaction potential between a particle and daughter nucleus are both changed due to the electron screening effect and their variations are both very important for the electron screening effect.Besides,the electron screening effect is found to be closely related to the decay energy and its proton number.
基金Supported by the National Natural Science Foundation of China(11822503,11575082,11947220)by the Fundamental Research Funds for the Central Universities(Nanjing University)+2 种基金by JSPS KAKENHI(JP18K03660,JP16K05351)by a Project funded by China Postdoctoral Science Foundation(2019M661785)The author N.W.would like to thank the support from the foreign young research support program in RCNP,Osaka University。
文摘Using bare Argonne V4'(AV4'),V6'(AV6'),and V8'(AV8')nucleon–nucleon(NN)interactions,the nuclear equations of state(EOSs)for neutron matter are calculated with the unitary correlation operator and high-momentum pair methods.Neutron matter is described using a finite particle number approach with magic number N=66 under a periodic boundary condition.The central short-range correlation originating from the short-range repulsion in the NN interaction is treated by the unitary correlation operator method(UCOM),and the tensor correlation and spin-orbit effects are described by the two-particle two-hole(2p2h)excitations of nucleon pairs,where the two nucleons with a large relative momentum are regarded as a high-momentum(HM)pair.With increasing 2p2h configurations,the total energy per particle of the neutron matter is well-converged under this UCOM+HM framework.Comparing the results calculated with AV4',AV6',and AV8'NN interactions,we demonstrate the effects of the short-range correlation,tensor correlation,and spin-orbit coupling on the density dependence of the total energy per particle of neutron matter.Moreover,the contribution of each Hamiltonian component to the total energy per particle is discussed.The EOSs of neutron matter calculated within the present UCOM+HM framework agree with the calculations of six microscopic many-body theories,especially the auxiliary field-diffusion Monte Carlo calculations.