共查询到20条相似文献,搜索用时 343 毫秒
1.
We studied the effect of Coulomb interaction on the isospin fractionation in the intermediate energy heavy ion collisions by using the isospin-dependent quantum molecular dynamics model. The calculated results show that Coulomb interaction induces the reduction of the isospin fractionation process with the evolutions of neutronproton ratio and mass of system. Because Coulomb interaction is repulsive for the proton, more binding protons become free, which produces the neutron-poor gas phase and neutron-rich liquid phase, compared to the neutronproton ratio of the system. The isospin fractionation degree is weakened by the Coulomb term. In contrast, the symmetry potential is repulsive for neutrons and attractive for protons in the neutron-rich system, and then the binding neutrons more than the protons become free, which produces a neutron-rich gas phase and neutron-poor liquid phase, so that the isospin fractionation degree is increased. The competition between the effects from the Coulomb interaction and the symmetry potential induces the reduction of the isospin fractionation degree for all the system masses. The properties for the sensitive dependence of isospin fractionation degree on the symmetry potential and weak dependence on the nucleon-nucleon cross section are preserved for all the neutron-rich systems. 相似文献
2.
Isospin Effect of Coulomb Interaction on Momentum Dissipation in Intermediate Energy Heavy Ion Collisions
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We investigate the isospin effect of Coulomb interaction on the momentum dissipation or nuclear stopping in the intermediate energy heavy ion collisions by using the isospin-dependent quantum molecular dynamics model. The calculated results show that the Coulomb interaction induces obviously the reductions of the momentum dissipation. We also find that the variation amplitude of momentum dissipation induced by the Coulomb interaction depends sensitively on the form and strength of symmetry potential. However, the isospin effect of Coulomb interaction on the momentum dissipation is less than that induced by the in-medium nucleon-nucleon cross section.In this case, Coulomb interaction does not change obviously the isospin effect of momentum dissipation induced by the in-medium two-body collision. In particular, the Coulomb interaction is preferable for standing up the isospin effect of in-medium nucleon-nucleon cross section on the momentum dissipation and reducing the isospin effect of symmetry potential on it, which is important for obtaining the feature about the sensitive dependence of momentum dissipation on the in-medium nucleon-nucleon cross section and weakly on the symmetry potential. 相似文献
3.
Nuclei offer an interesting isospin situation where symmetry potential, Coulomb term and isopin dependent nucleon-nucleon collisions are simultaneously present. However, in general, Coulomb potential is not studied in the heavy ion collisions. As we know that the Coulomb potential is an important asymmetry term which can bring important isospin effect into the observable in the intermediate energy heavy ion collisions. Recently extensions by Colonna et al.[1] to finite nuclei show that Coulomb and surface effects reduce instability regions. So in this paper the isospin effects of Coulomb term and symmetry potential on the nuclear stopping at intermediate energy heavy ion collisions are studied by using isospin-dependent quantum molecular dynamics model (IQMD). 相似文献
4.
Relativistic effect of pseudospin symmetry and tensor coupling on the Mie-type potential via Laplace transformation method
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A relativistic Mie-type potential for spin-1/2 particles is studied. The Dirac Hamiltonian contains a scalar S(r) and a vector V(r) Mie-type potential in the radial coordinates, as well as a tensor potential U(r) in the form of Coulomb potential. In the pseudospin(p-spin) symmetry setting Σ = Cps and Δ = V(r), an analytical solution for exact bound states of the corresponding Dirac equation is found. The eigenenergies and normalized wave functions are presented and particular cases are discussed with any arbitrary spin–orbit coupling number κ. Special attention is devoted to the caseΣ = 0 for which p-spin symmetry is exact. The Laplace transform approach(LTA) is used in our calculations. Some numerical results are obtained and compared with those of other methods. 相似文献
5.
The model of the Coulomb dressed potential is applied to solving the
problem of electron scattering for simplifying the calculation in the
electrostatic field and the excimer laser field. The introduction and
the application of the model are based on the electric dipole
approximation, so the contribution of the electric multipole is
neglected. In this paper, rigorous analysis and deduction are
carried out for the introduction of the dressed Coulomb potential
into the laser field. It is found that the introduction of the
dressed potential in the fractional form is feasible only when the
laser field (not including far ultraviolet field and x-ray) is a weak
field, i.e. the quiver radius of the free electron is smaller than
the atomic scale. In addition, the necessary analysis is also
conducted of the limitation of the application of the Coulomb dressed
potential. 相似文献
6.
This paper presents the dynamical properties of a Rydberg hydrogen atom between two metal surfaces using phase space analysis methods. The dynamical behaviour of the excited hydrogen atom depends sensitively on the atom--surface distance d. There exists a critical atom--surface distance dc = 1586 a.u. When the atom--surface distance d is larger than the critical distance dc, the image charge potential is less important than the Coulomb potential, the system is near-integrable and the electron motion is regular. As the distance d decreases, the system will tend to be non-integrable and unstable, and the electron might be captured by the metal surfaces. 相似文献
7.
Based on both very obvious isospin effect of the neutron-proton number ratio of nucleon emissions (n/p)nud on symmetry potential and (n/p)nucl's sensitive dependence on symmetry potential in the nuclear reactions induced by halo-neutron projectiles, compared to the same mass stable projectile, probing symmetry potential is investigated within the isospin-dependent quantum molecular dynamics with isospin and momentum-dependent interactions for different symmetry potentials U;ym and U2^sym. It is found that the neutron-halo projectile induces very obvious increase of (n/p)nucl and strengthens the dependence of (n/p) l on the symmetry potential for all the beam energies and impact parameters, compared to the same mass stable projectile under the same incident channel condition. Therefore (n/p)nucl induced by the neutron-halo projectile is a more favourable probe than the normal neutron-rich and neutron-poor projectiles for extracting the symmetry potential. 相似文献
8.
Pseudoscalar Cornell potential for a spin- 1/2 particle under spin and pseudospin symmetries in 1 + 1 dimension
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The Cornell potential that consists of Coulomb and linear potentials has received a great deal of attention in particle physics. In this paper, we present the exact solutions of the Dirac equation with the pseudoscalar Cornell potential under spin and pseudospin symmetry limits. The energy eigenvalues and corresponding eigenfunctions are given in closed form. 相似文献
9.
LIU Chao XIE Wen-Fang 《理论物理通讯》2009,51(2):353-357
In this paper we study a negatively charged exciton (NCE), which is trapped by a two-dimensional (2D) parabolic potential. By using matrix diagonalization techniques, the correlation energies of the low-lying states with L=0, 1, and 2 are calculated as a function of confinement strength. We find that the size effects of different states are different. This phenomenon can be explained as a hidden symmetry, which is originated purely from symmetry. Based on symmetry, the features of the low-lying states are discussed in the influence of the 2D parabolic potential well. It is found that the confinement may cause accidental degeneracies between levels with different low-excited states. It is shown that the effect of quantum confinement on the binding energy of the heavy hole is stronger than that of a light hole. 相似文献
10.
High-order harmonic generation spectrum of an excited one-dimensional Coulomb atom in an intense laser field
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Response of the wave packet of a one-dimensional Coulomb atom
to an intense laser field is calculated using the symmetrized
split operator fast Fourier method. The high-order harmonic
generation (HHG) of the initial state separately being the ground and excited states
is presented. When the hardness parameter \alpha in the soft
Coulomb potential V(x)=-1/\sqrt{x^2+\alpha} is chosen to be small
enough, the so-called hard Coulomb potential
V(x)=-1/|x| can be obtained. It is well known that the hard one-dimensional Coulomb atom
has an unstable ground
state with an energy eigenvalue of $\sim0.5$ and it
has no states corresponding to physical states in the true atoms, and
has the first and second excited states being degenerate. The parity effects on the HHG
can be seen from the first and second excited states of the hard
one-dimensional Coulomb atom. The HHG spectra of the excited states
from both the soft and hard Coulomb atom models are shown to have more
complex structures and to be much stronger than the corresponding
HHG spectrum of the ground state of the soft Coulomb model with
$\alpha=2$ in the same laser field. Laser-induced non-resonant
one-photon emission is also observed. 相似文献
11.
在C60分子中,未被填充的最低电子态具有T1u对称性,因此,对中性的C60而言,不论是通过分子内部激发,或是外部掺杂,都易被一个电子占据而形成Jahn-Teller(JT)活跃电子态.此态与五重简并的hg声子态耦合,构成所谓的T1u-hg -JT系统.在这一JT系统中,当只考虑电声的线性耦合时,其绝热势能面是一个槽形.但在实际的系统中,二阶电声耦合是存在的,理论研究表明,原来的势槽将被这二阶非线性耦合弯曲成D3d或D5d对称性的势阱.声子振动态在阱中将显示各向异性效应,使得声子沿不同的方向有不同的振动频率,进而影响势阱中的能级分布、势阱间的重叠积分,以及整个系统的隧道能级分裂等.对D3d势阱中各向异性效应进行了研究,利用幺正平移、?pik Pryce和标度变换等方法计算了系统势阱中的能级,以及阱中的振动频率,研究了势阱中的能级间隔以及微绕修正能量的变化,并由此导出了这些物理量在仅有线性耦合的势槽中变化的情形.
关键词:
C60
Jahn-Teller效应
各向异性
电声耦合 相似文献
12.
Using angle-resolved photoemission spectroscopy utilizing polarized synchrotron radiation with a clean Fe(110) sample, we identified each of the Σ1-, Σ3- and Σ4-band peaks with certainty using symmetry selection rules. We also determined energy band dispersion along the γ-Σ-N direction in the bulk Brillouin zone assuming direct transitions. There are small discrepancies between the observed bands and recent ground-state band calculations possibly due to Coulomb correlation effects. A surface state with odd symmetry about the [001] crystal direction and a binding energy of 0.15 eV at γ in the surface Brillouin zone was observed. Our results show that the ground-state calculations of ferromagnetic iron based on the local exchange correlation potential are basically in agreement with experimental dispersion relationship measurements. 相似文献
13.
在AdS5S5背景中,IIB超弦的运动方程与Maurer-Cartan方程在世界面上存在对偶对称性.通过引入扭曲对偶(twisteddual)的概念,将有限的对偶变换推广到连续的对偶变换,并给出了AdS5S5中IIB超弦的Lax联络及其可积的相容条件.
关键词:
扭曲对偶
κ对称性
Lax联络 相似文献
14.
We give generalizations of extended Poincaré supergravity with arbitrarily many supersymmetries in the absence of central charges in three dimensions by gauging its intrinsic global SO(N) symmetry. We call these 0 (Aleph-null) supergravity theories. We further couple a non-Abelian supersymmetric Chern-Simons theory and an Abelian topological BF theory to 0 supergravity. Our result overcomes the previous difficulty for supersymmetrization of Chern-Simons theories beyond N = 4. This feature is peculiar to the Chern-Simons and BF theories including supergravity in three dimensions. We also show that dimensional reduction schemes for four-dimensional theories such as N = 1 self-dual supersymmetric Yang-Mills theory or N = 1 supergravity theory that can generate 0 globally and locally supersymmetric theories in three dimensions. As an interesting application, we present 0 supergravity Liouville theory in two dimensions after appropriate dimensional reduction from three dimensions. 相似文献
15.
《Nuclear Physics B》2001,600(3):620
The semi-classical limit of the algebraic Bethe ansatz method is used to solve the theory of Gaudin models. Via off-shell Bethe ansatz method we find the spectra and eigenvectors of the N−1 independents Gaudin Hamiltonians with symmetry osp(21). We also show how the off-shell Gaudin equation solves the trigonometric Knizhnik–Zamolodchikov equation. 相似文献
16.
18.
We update the study of the QCD corrections to direct J/ψ and hadroproduction in association with a photon in the QCD-based approach of the Colour-Singlet (CS) Model. After comparison with the recent full next-to-leading-order (NLO) computation for this process, we provide an independent confirmation to the inclusive case that NLO QCD corrections to quarkonium-production processes whose LO exhibits a non-leading PT behaviour can be reliably computed at mid and large PT by considering only the real emission contributions accompanied with a kinematical cut. In turn, we evaluate the leading part of the contributions, namely those coming from (J/ψ,)+γ associated with two light partons. We find that they are dominant at mid and large PT. This confirms our expectations from the leading PT scaling of the new topologies appearing at NNLO. We obtain that the yield from the CS becomes one order of magnitude larger than the upper value of the potential colour-octet yield. The polarisation of the quarkonia produced in association with a photon is confirmed to be longitudinal at mid and large PT. 相似文献
19.
We obtain the one-loop quantum corrections to the Kählerian and superpotentials in the generic chiral superfield model on the nonanticommutative superspace. Unlike all previous works, we use a method which does not require to rewrite a star-product of superfields in terms of ordinary products. In the Kählerian potential sector the one-loop contributions are analogous to ones in the undeformed theory while in the chiral potential sector the quantum corrections contain a deformation parameter. 相似文献