A photonuclear reaction transport model based on an isospin-dependent quantum molecular dynamics model （IQMD） is presented in the intermediate energy region, which is named as GiQMD in this study. Methodology to sim...A photonuclear reaction transport model based on an isospin-dependent quantum molecular dynamics model （IQMD） is presented in the intermediate energy region, which is named as GiQMD in this study. Methodology to simulate the course of the photonuclear reaction within the IQMD frame is described to study the photo- absorption cross section and π meson production, and the simulation results are compared with some available experimental data as well as the Giessen Boltzmann-Uehling-Uhlenbeck model.展开更多
A potential version of the UrQMD(UrQMD/M) transport model and a traditional coalescence model are combined to calculate the production of ~3He fragments in central Pb+Pb collisions at SPS energies 20-80 Ge V/nucleon. ...A potential version of the UrQMD(UrQMD/M) transport model and a traditional coalescence model are combined to calculate the production of ~3He fragments in central Pb+Pb collisions at SPS energies 20-80 Ge V/nucleon. It is found that the Lorentz transformation in the afterburner influences visibly the ~3He yield and should be considered in calculations. The rapidity distribution of ~3He multiplicities(including the concave shape) can be described well with Ur QMD/M when it stops during t_cut=(100±25) fm/c and the coalescence afterburner with one parameter set of(R_0,P_0)=(3.8 fm, 0.3 Ge V/c) is taken into use afterwards.展开更多
Rapidity distributions of both E895 proton data at AGS energies and NA49 net proton data at SPS energies can be described reasonably well with a potential version of the Ur QMD in which mean-field potentials for both ...Rapidity distributions of both E895 proton data at AGS energies and NA49 net proton data at SPS energies can be described reasonably well with a potential version of the Ur QMD in which mean-field potentials for both pre-formed hadrons and confined baryons are considered, with the help of a traditional coalescence afterburner in which one parameter set for both relative distance R_0 and relative momentum P_0,(3.8 fm, 0.3 Ge V/c), is used. Because of the large cancellation between the expansion in R_0 and the shrinkage in P_0 through the Lorentz transformation, the relativistic effect in clusters has little effect on the rapidity distribution of free(net) protons. Using a Woods-Saxon-like function instead of a pure logarithmic function as seen by FOPI collaboration at SIS energies, one can fit well both the data at SIS energies and the Ur QMD calculation results at AGS and SPS energies. Further, it is found that for central Au+Au or Pb+Pb collisions at top SIS, SPS and RHIC energies, the proton fractions in clusters are about33%, 10%, and 0.7%, respectively.展开更多
The time evolution of both proton and anti-proton v_2 flows from Au+Au collisions at (S_NN)^(1/2)=7.7 Ge V are examined by using both pure cascade and mean-field potential versions of the Ur QMD model. Due to a strong...The time evolution of both proton and anti-proton v_2 flows from Au+Au collisions at (S_NN)^(1/2)=7.7 Ge V are examined by using both pure cascade and mean-field potential versions of the Ur QMD model. Due to a stronger repulsion at the early stage introduced by the repulsive potentials and hence much less annihilation probabilities, anti-protons are frozen out earlier with smaller v_2 values.Therefore, the experimental data of anti-proton v_2 as well as the flow difference between proton and anti-proton can be reasonably described with the potential version of UrQMD.展开更多
应用一种扩展的分子动力学模型(Extension of quantum molecular dynamics,EQMD)研究了轻核的晕结构和团簇结构。对于晕结构,详细讨论了晕结构核在EQMD模型框架下的初始化,给出了14Be、17B、19C和22C的晕核结构性质和物质密度分布,讨论...应用一种扩展的分子动力学模型(Extension of quantum molecular dynamics,EQMD)研究了轻核的晕结构和团簇结构。对于晕结构,详细讨论了晕结构核在EQMD模型框架下的初始化,给出了14Be、17B、19C和22C的晕核结构性质和物质密度分布,讨论了价中子波包宽度、核芯核子的波包宽度以及核芯的形态对于晕结构存在的重要性。对于团簇结构,给出了EQMD模型框架下对于轻的4n核的α团簇态的描述结果,讨论了不同团簇态的稳定性、结合能以及不同核子的波包宽度,指出了团簇态在自由演化过程中的α之间能量流动性质。并讨论了4-α正四面体结构作为16O基态的可能性。展开更多
基金Supported by the National Natural Science Foundation of China under Grant Nos 11421505 and 11220101005the National Basic Research Program of China under Grant No 2014CB845401the Strategic Priority Research Program of the Chinese Academy of Sciences under Grant No XDB16
文摘A photonuclear reaction transport model based on an isospin-dependent quantum molecular dynamics model （IQMD） is presented in the intermediate energy region, which is named as GiQMD in this study. Methodology to simulate the course of the photonuclear reaction within the IQMD frame is described to study the photo- absorption cross section and π meson production, and the simulation results are compared with some available experimental data as well as the Giessen Boltzmann-Uehling-Uhlenbeck model.
基金the National Natural Science Foundation of China(Grant Nos.11375062,11275068,11505056,and 11505057)the project sponsored by SRF for ROCS,SEM,the Education Bureau of Zhejiang Province(Grant No.Y201533176)the Doctoral Scientific ResearchFoundation(Grant No.11447109)
文摘A potential version of the UrQMD(UrQMD/M) transport model and a traditional coalescence model are combined to calculate the production of ~3He fragments in central Pb+Pb collisions at SPS energies 20-80 Ge V/nucleon. It is found that the Lorentz transformation in the afterburner influences visibly the ~3He yield and should be considered in calculations. The rapidity distribution of ~3He multiplicities(including the concave shape) can be described well with Ur QMD/M when it stops during t_cut=(100±25) fm/c and the coalescence afterburner with one parameter set of(R_0,P_0)=(3.8 fm, 0.3 Ge V/c) is taken into use afterwards.
基金the National Natural Science Foundation of China(Grant Nos.1137506211547312 and 11275068)+2 种基金the project sponsored by SRF for ROCSSEMand the Doctoral Scientific Research Foundation(Grant No.11447109)
文摘Rapidity distributions of both E895 proton data at AGS energies and NA49 net proton data at SPS energies can be described reasonably well with a potential version of the Ur QMD in which mean-field potentials for both pre-formed hadrons and confined baryons are considered, with the help of a traditional coalescence afterburner in which one parameter set for both relative distance R_0 and relative momentum P_0,(3.8 fm, 0.3 Ge V/c), is used. Because of the large cancellation between the expansion in R_0 and the shrinkage in P_0 through the Lorentz transformation, the relativistic effect in clusters has little effect on the rapidity distribution of free(net) protons. Using a Woods-Saxon-like function instead of a pure logarithmic function as seen by FOPI collaboration at SIS energies, one can fit well both the data at SIS energies and the Ur QMD calculation results at AGS and SPS energies. Further, it is found that for central Au+Au or Pb+Pb collisions at top SIS, SPS and RHIC energies, the proton fractions in clusters are about33%, 10%, and 0.7%, respectively.
基金the National Natural Science Foundation of China(Grant Nos.1137506211547312,and 11275068)the project sponsored by SRF for ROCS,SEM,and the Doctoral Scientific Research Foundation(Grant No.11447109)
文摘The time evolution of both proton and anti-proton v_2 flows from Au+Au collisions at (S_NN)^(1/2)=7.7 Ge V are examined by using both pure cascade and mean-field potential versions of the Ur QMD model. Due to a stronger repulsion at the early stage introduced by the repulsive potentials and hence much less annihilation probabilities, anti-protons are frozen out earlier with smaller v_2 values.Therefore, the experimental data of anti-proton v_2 as well as the flow difference between proton and anti-proton can be reasonably described with the potential version of UrQMD.
文摘应用一种扩展的分子动力学模型(Extension of quantum molecular dynamics,EQMD)研究了轻核的晕结构和团簇结构。对于晕结构,详细讨论了晕结构核在EQMD模型框架下的初始化,给出了14Be、17B、19C和22C的晕核结构性质和物质密度分布,讨论了价中子波包宽度、核芯核子的波包宽度以及核芯的形态对于晕结构存在的重要性。对于团簇结构,给出了EQMD模型框架下对于轻的4n核的α团簇态的描述结果,讨论了不同团簇态的稳定性、结合能以及不同核子的波包宽度,指出了团簇态在自由演化过程中的α之间能量流动性质。并讨论了4-α正四面体结构作为16O基态的可能性。
