W含温有界下状态方程参数的理论计算

在改进的Hartree-Fock-Slater原子模型的基础上,在中心场近似下用含能带效应的全动态电子判据处理自由电子与束缚电子的密度分布,提高了电子波函数、电子占据数等原子参数的计算精度.通过平均近似处理,给出了劈裂的能带,从而改善了物质电子状态方程的计算精度.结果部分详细计算了W元素的原子能量、电子压强、熵、定容热容及其它热力学参数     

Au等离子体电子状态方程的理论研究

在改进的平均原子模型的基础上,在中心场近似下用分波法来处理部分自由电子密度分布函数,提高了电子波函数、电子占据数等原子参数的计算精度.通过平均近似处理,给出了劈裂的能带.通过使用分波法来准确计算贵金属Au的电子状态方程.     

包含过渡区的等离子体电子状态方程的理论研究

在改进的平均原子模型的基础上,在中心场近似下用分波法来处理部分自由电子密度分布函数,提高了电子波函数、电子占据数等原子参数的计算精度.通过平均近似处理,给出了劈裂的能带,从而改善了物质电子状态方程的计算精度.作为算例,计算了Mo,Au等元素的原子能量、电子压强、熵及定容热容. 关键词： 自洽场原子结构 原子能量     

Au等离子体电子状态方程的理论研究

在改进的平均原子模型的基础上，在中心场近似下用分波法来处理部分自由电子密度分布函数，提高了电子波函数、电子占据数等原子参数的计算精度．通过平均近似处理，给出了劈裂的能带．通过使用分波法来准确计算贵金属Au的电子状态方程．     

改进的含温有界原子模型对金的电子物态方程的计算

在改进的含温有界原子模型基础上,在中心场近似下用分波法来处理部分自由电子密度分布函数.通过平均近似处理,给出劈裂的能带.在原子结构的自洽计算中采用能带重叠作为自由电子的动态判据.大量计算了Au的电子压强、能量、热容以及各种热力学系数. 关键词： 自洽场原子结构 状态方程 原子能量 电子压强     

中低温等离子体原子能量的分波法计算

在改进的平均原子模型的基础上，在中心场近似下用分波法处理自由电子密度分布函数，提高了电子波函数、电子占据数等原子参数的计算精度.通过使用分波法准确计算电子间各部分的相互作用能，使得原子能量的计算结果更加准确，零温基态能的计算结果与Hartree-Fock理论给出的结果很好地符合.作为算例，计算了W，Au，Rn，Am等元素的原子能量、熵及定容热容. 关键词： 自洽场原子结构 原子能量     

第一原理研究界面弛豫对InAs/GaSb超晶格界面结构、能带结构和光学性质的影响

通过广义梯度近似的第一原理全电子相对论计算, 研究了不同界面类型InAs/GaSb超晶格的界面结构、电子和光吸收特性. 由于四原子界面的复杂性和低对称性, 通过对InAs/GaSb超晶格进行电子总能量和应力最小化来确定弛豫界面的结构参数. 计算了InSb, GaAs型界面和非特殊界面(二者交替)超晶格的能带结构和光吸收谱, 考察了超晶格界面层原子发生弛豫的影响.为了证实能带结构的计算结果, 用局域密度近似和Hartree-Fock泛函的平面波方法进行了计算. 对不同界面类型InAs/GaSb超晶格的能带结构计算结果进行了比较, 发现界面Sb原子的化学键和离子性对InAs/GaSb超晶格的界面结构、 能带结构和光学特性起着至关重要的作用.     

用线性丸盒轨道原子球近似超元胞法计算(Ba_(1-x)K_x)BiO_3立方超导相(x=0.25,0.5,0.75)的电子结构

用线性丸盒轨道原子球近似(LMTO-ASA)超元胞法计算(Ba_(1-x)Kx)BiO_3立方超导相x=0.25与x=0.5的电子结构,作为对照同时计算立方结构x=0.75的电子结构。计算结果表明,用超元胞法可以得到比“刚带近似”较精确的电子结构参数。给出Fermi面上的能带参数随组分的变化趋势。讨论了不等价的氧原子与周围金属原子价轨道的杂化特征。     

用线性丸盒轨道原子球近似超元胞法计算(Ba1-xKx)BiO3立方超导相(x=0.25,0.5,0.75)的电子结构

用线性丸盒轨道原子球近似(LMTO-ASA)超元胞法计算(Ba_1-xKx)BiO₃立方超导相x=0.25与x=0.5的电子结构,作为对照同时计算立方结构x=0.75的电子结构。计算结果表明,用超元胞法可以得到比“刚带近似”较精确的电子结构参数。给出Fermi面上的能带参数随组分的变化趋势。讨论了不等价的氧原子与周围金属原子价轨道的杂化特征。 关键词：     

非平衡等离子体中原子过程的计算

为得到由中、高Z元素形成的非局域热动平衡等离子体中的离子丰度分布的可靠信息 ,对建立速率方程所需的各种离子的各个原子过程采用了基于一级微扰论的计算 ,提高了原子参数的精度 ;为了进一步节省计算时间 ,在保证精度的前提下 ,针对不同的过程做了不同的近似处理 ;对各个原子过程的计算结果进行多方比较,表明精度可靠.     

Photoionization of some closed shell atoms and ions

Dipole-allowed single photoionization of some closed shell atoms and ions has been investigated in the relativistic random-phase approximation (RRPA). Application of relativisticmultichannel quantum defect theory (RMQDT) is made together with RRPA to analyse autoionizing resonances. Analysis points to the importance of interchannel coupling in high energy photoionization and reveals various degeneracies in relativistic atomic spectra to influence the low energy dynamics. Interesting threshold behavior in photoelectron spin polarization has been seen. Prospective future studies have been indicated.     

铑原子基态的理论研究

在有心力场近似和组态相互作用理论框架下,通过对电子波函数、各个壳层上电子的束缚能、平均轨道半径、总束缚能、基组态时的激发能、电离能的分析和计算,研究了Lr原子的可能基组态及其基组态时的原子态.研究结果表明:基组态为5f147s27p,基态时的原子态为2P1/2.     

空心光纤中LP01模的场分布

本文用弱导光纤近似分析了空心光纤LP01模的场分布,得出了色散方程,并进行了数值计算.     

Laser-Assisted particle-atom inelastic collisions. Role of the field polarization

Summary A theoretical treatment, of first order in the collision dynamics, is presented to analyse the role of electric polarization in offresonance laser-assisted atomic collisions. General expressions are presented for evaluating the modified spectrum and wave functions for anyn level of hydrogenic atoms in the presence of a laser, taken to be linearly and circularly polarized. Specific calculations are carried out for excitation of hydrogen atoms to the leveln=2 by electron impact. The two polarizations are found to yield large differences i) in the atomic-spectrum modifications, ii) in the structure of the cross-sections and iii) in the numerical results. In particular, only for linear polarization, the distribution in energy of the scattered electrons at a fixed scattering angle has the structure of a series of equally spaced lines of different height (the spacing being equal to the laser photon energy ℏw and the height of the line accounting for the number of final electrons with a given energy). For circular polarization no such a regular pattern is predicted. Since, among laser-assisted particle-atom collisions, at present energy gain-loss spectra of scattered electrons are most easily observed, it is hoped that the reported results may serve as a stimulus for new observations in this new class of atomic collisions. The theory to treat the multiphoton resonance case is outlined too. To speed up publication, the authors of this paper have agreed to not receive the proofs for correction.     

Local charge-carrier trapping centers in C60 single crystals

The energy spectrum of local charge-carrier trapping centers in C₆₀ single crystals is studied in terms of the theory of space-charge-limited currents in the Gaussian approximation. The energy distribution of these centers in the energy gap is found, and the type and parameters of this distribution are determined.     

Adiabatic description of impenetrable particles in an infinitely deep potential well

In the framework of adiabatic approximation the energy spectrum and wave functions of two impenetrable particles in an infinitely deep potential well are considered for two cases of approximation of the effective confining potential of the ??slow?? subsystem. In case of the quadraticterm approximation the obtained energy spectrum is equidistant. The probability distribution in the range of ??fast?? particle has a symmetric shape while that in the range of the ??slow?? particle is asymmetric and the peak of localization of the system in its ground state is shifted towards the ??fast?? particle. In the first excited state the center of the probability distribution of the ??slow?? particle is shifted towards the impenetrable wall.     

系综分布和它的小涨落近似

由“从正则分布出发，在小涨落近似下得出的能量涨落分布公式”求得的能量涨落的二次矩与直接由正则分布求得的二次矩完全相同，但分别由二求得的高次矩并不完全相同。     

Comparisons between statistics of low energy collision cascades generated by full molecular dynamics and by its binary collision approximation

Abstract

Collision cascades in Cu, Au and Cu₃Au are generated by full molecular dynamics (MD) and by its binary collision approximation (BCA) with the Marlowe program. Cu and Au primaries have 1 keV initial energy.

The same Molière repulsive potential is used in both models for close encounters. In the MD model, this potential is carefully splined to the pair component of the N-body potential developed by Ackland and Vitek. In the BCA, this N-body interaction is roughly modeled by a constant isotropic 4 eV binding energy of the target atoms to their rest positions.

Time distributions of the number of atoms moving with a total energy higher than a threshold value E _d are compared and discussed. Recoil range distributions during the cascade development are discussed as well. The agreement between MD and BCA is fairly good in all cases for E _d larger than about 3 eV. In the case of smaller E _d-values, the BCA may result in an overestimate of the number of moving atoms in the late development of the cascades. This discrepancy is suggested to originate in the lack of attractive forces between the moving particles and the surrounding atoms in the BCA.