共查询到19条相似文献,搜索用时 796 毫秒
1.
2.
3.
4.
本文运用密度泛函理论的B3LYP方法, 对钚原子应用LANL2DZ收缩价基函数, 氮、氧原子采用AUG-cc-pVTZ基函数, 分别对PuN, PuO, NO和PuNO体系进行了结构优化, 得到PuNO分子最稳构型为C∞v (Pu-N-O), 电子态为6Σ- (基态), 平衡核间距RON=0.12257 nm, RNPu=0.22951 nm, 离解能De=8.10537 eV. 同时优化得到PuNO 分子存在两种亚稳态平衡构型分别为C∞v (Pu-O-N), 6Σ- (电子态)和Cs (O-Pu-N), A" (电子态), 以及分子体系相应的力学常数等. 拟合出PuN, PuO 和NO 分子的Murrell-Sorbie势能函数, 并使用多体项展式理论得到了PuNO分子的分析势能函数, 其等值势能图准确再现了PuNO分子最稳态构型及两个亚稳态构型的离解能和结构特性, 由此讨论了该分子体系的势能面静态特征. 相似文献
5.
运用密度泛函理论下的广义梯度近似和交换关联函数对Cu吸附(SiO2)n(n=1—8)团簇的几何结构、电荷分布、稳定性和电子性质进行了较详细的研究,结果表明: Cu原子易于和带有悬挂键的Si原子作用并形成"铜岛膜"; Cu吸附(SiO2)n团簇后Si原子失去电子能力减弱,O原子得到电子能力增强;Cu(SiO2)n(n
关键词:
密度泛函理论
2)n (n=1—8)团簇')" href="#">Cu(SiO2)n (n=1—8)团簇
近红外吸收 相似文献
6.
7.
8.
本文由粘滞系数的时间关联函数表达式,得到了实验观察到的现象:在液晶N相→SA相转变点附近(T→T(sA)),体粘滞系数的反常发散比切变粘滞系数反常发散要大得多。说明了Brochard等人的理论中,不能解释此实验的原因。
关键词: 相似文献
9.
10.
利用分子动力学方法,模拟了5000个表面轻微摩擦(μ=1×10-4)的弹性颗粒组成的体系在各向同性压缩过程中的堵塞(jamming)现象,研究了颗粒体系对边壁压强P和对关联函数第一个峰的高度g1随体积分数φ的变化规律. 结果表明,当体系的体积分数φ大于临界体积分数φc时,P(φ)曲线表现出明显的黏滑(stick-slip)行为,法向的力-力关联函数、切向的力-力关联函数和颗粒的位置-位置关联函数同时发生跳变,说明宏观黏滑现象源自内部的力位形和几何构形的调整. 体系在φ缓慢增大过程中得到了不同的堵塞态,随着颗粒粒径的缓慢减小,体系得以松弛(unjamming),实现松弛过程并得到相应的φc. 对于不同堵塞态,其边壁压强P与φ-φc遵从幂律标度P∝(φ-φc)0.964.
关键词:
堵塞相图
对关联函数
力-力关联函数
标度规律 相似文献
11.
12.
R. R. Nigmatullin A. A. Khamzin I. I. Popov 《Journal of Experimental and Theoretical Physics》2012,114(2):314-323
We suggest a new method of calculation of the equilibrium correlation functions of an arbitrary order for the interacting
Fermi-gas model in the framework of the static fluctuation approximation method. This method based only on a single and controllable
approximation allows obtaining the so-called far-distance equations. These equations connecting the quantum states of a Fermi
particle with variables of the local field operator contain all necessary information related to the calculation of the desired
correlation functions and basic thermodynamic parameters of the many-body system. The basic expressions for the mean energy
and heat capacity for the electron gas at low temperatures in the high-density limit were obtained. All expressions are given
in the units of r
s
, where r
s
determines the ratio of a mean distance between electrons to the Bohr radius a
0. In these expressions, we calculate terms of the respective order r
s
and r
s
2. It is also shown that the static fluctuation approximation allows finding the terms related to higher orders of the decomposition
with respect to the parameter r
s
. 相似文献
13.
《Surface science》1987,182(3):423-430
A study of the influence of many-body effects on binding energies and effective masses of image potential induced surface states is presented. The binding energies calculated using experimentally measured ε(ω) response functions show a dependence on the electron density different from that obtained using a plasmon model, and are in agreement with recent experimental data of diesen et al. [Phys. Rev. B33 (1986) 5241]. The effects of plasmon dispersion and single particle excitations on binding energies are evaluated with a simple model, and it is shown that they result in a strong cancellation in the range of rs values where most experimental data have been obtained (rs ≈ 3), if realistic values of the surface plasmon dispersion relation are used. Corrections to the effective masses due to many-body effects are shown to be of the order of 1%. 相似文献
14.
15.
A. Gold 《Zeitschrift für Physik B Condensed Matter》1992,86(2):193-206
For a superlattice with periodd the Singwi et al. (Phys. Rev.176, 589 (1968)) approach for the local-field correction and the static structure factor is formulated. With two approximations we reduce the resulting three-dimensional integral-equation into a one-dimensional integral-equation. For the local-field correction we present analytical results for small wave numbers and large wave numbers. An expression of Hubbard-typ is derived for the local-field correction. Explicit results for boson superlattices and electron superlattice are given. A charge-density-wave instability in a layered Bose condensate withr
s>rscd3/4 is discovered.r
s
is the small parameter of the random-phase-approximation. The charge-density-wave instability is due to a many-body anomaly (short-range correlations) in layered structures and is a general property of layered quantum liquids. We find the charge-density-wave instability in a layered electron gas forr
s>rscd. Double-quantum-well structures are also considered. The effects of a finite well width is calculated. The general implications of the charge-density-wave instability for microscopically layered quantum liquids are pointed out. 相似文献
16.
17.
P. J. Forrester 《Journal of statistical physics》1993,72(1-2):39-50
In a previous paper the two-particle distribution function and one-particle density matrix for the quantum many-body system with the 1/r
2 pair potential have been expressed as limiting cases of Selberg correlation integrals. Recurrence equations are derived which allow rapid evaluation of these multidimensional integrals. The exact results for the two-particle distribution are compared with the harmonic approximation. 相似文献
18.
S. V. Shevkunov 《Journal of Experimental and Theoretical Physics》2006,103(1):92-109
Thermally excited states of the three-dimensional electron gas in a neutralizing background are computed by path integral Monte Carlo simulation for values of the Wigner-Seitz radius within the interval 5 < r s < 15. Coulomb and exchange interactions, permutation symmetry, and spin state are treated explicitly. Variation of electron correlation functions with density and temperature is analyzed. Quantum effects suppress and enhance spatial correlation at low and high densities, respectively. Transition between the electron-gas states characterized by these opposite trends corresponds to a density of approximately 2.5 × 1021 cm?3. A transition line between liquid-like and gaslike phases is determined in the temperature-density diagram. Weak anisotropy of many-body correlations in the liquid-like state stimulates excitation of spherically symmetric collective rotational modes. The effective short-range pseudopotential exhibits strong temperature dependence due to exchange effects. For strongly correlated systems, the characteristic screening length deviates from that predicted by the Thomas-Fermi screening model ( $ \sim \sqrt {r_s } $ ), approaching a linear function of r s. The effective short-range interaction substantially differs from the Yukawa potential in mean field theory. Coulomb interaction shifts the Fermi level up by an order of magnitude or higher, and this effect becomes stronger with decreasing density. 相似文献
19.
We present calculations of the spin-averaged pair distribution function g(r) in a homogeneous gas of electrons moving in dimensionality D=3 or D=2 at finite temperature. The model involves the solution of a two-electron scattering problem via an effective potential, which embodies many-body effects through a self-consistent Hartree approximation, leading to two-body wave functions to be averaged over a temperature-dependent distribution of relative momentum for electron pairs. We report illustrative numerical results for g(r) in an intermediate-coupling regime and interpret them in terms of changes of short-range order with increasing temperature. 相似文献