摘要翻译:
本文是前文[L.{v{S}}amaj和B.Jancovici,2007{it J.stat.mech.}P02002]的继续;对于平面硬壁(无像力)约束的半空间中的近似经典量子流体,我们推广了平衡点统计量的Wigner-Kirkwood展开式。作为一个更详细研究的模型系统,我们考虑量子二维单组分等离子体:一种带电粒子通过二维对数库仑势相互作用,在相反符号的均匀带电背景中,使总电荷消失。对应的经典系统在各种几何条件下都是精确可解的,包括现在的半平面,当$βe2=2$时,其中$β$是逆温度,$e$是粒子的电荷:所有的经典$n$-体密度都是已知的。对于量子单组分等离子体,通过启发式宏观论证,很久以前就已经导出了两个关于截断二体密度(其中一个是密度分布)的求和规则:一个是关于截断二体密度沿壁的渐近形式的求和规则,另一个是关于结构因子的偶极矩的求和规则。在$\betae^2=2$的二维情形下,我们现在有了这两个量子密度的$\hbar^2$级的显式表达式,因此我们可以在微观上检查这个级的和规则。检查是积极的,加强了求和规则是正确的想法。
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英文标题:
《Correlations and sum rules in a half-space for a quantum two-dimensional
one-component plasma》
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作者:
B. Jancovici, L. Samaj
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最新提交年份:
2007
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分类信息:
一级分类:Physics 物理学
二级分类:Statistical Mechanics 统计力学
分类描述:Phase transitions, thermodynamics, field theory, non-equilibrium phenomena, renormalization group and scaling, integrable models, turbulence
相变,热力学,场论,非平衡现象,重整化群和标度,可积模型,湍流
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一级分类:Physics 物理学
二级分类:Quantum Physics 量子物理学
分类描述:Description coming soon
描述即将到来
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英文摘要:
This paper is the continuation of a previous one [L. {\v{S}}amaj and B. Jancovici, 2007 {\it J. Stat. Mech.} P02002]; for a nearly classical quantum fluid in a half-space bounded by a plain plane hard wall (no image forces), we had generalized the Wigner-Kirkwood expansion of the equilibrium statistical quantities in powers of Planck's constant $\hbar$. As a model system for a more detailed study, we consider the quantum two-dimensional one-component plasma: a system of charged particles of one species, interacting through the logarithmic Coulomb potential in two dimensions, in a uniformly charged background of opposite sign, such that the total charge vanishes. The corresponding classical system is exactly solvable in a variety of geometries, including the present one of a half-plane, when $\beta e^2=2$, where $\beta$ is the inverse temperature and $e$ is the charge of a particle: all the classical $n$-body densities are known. For the quantum one-component plasma, two sum rules involving the truncated two-body density (and, for one of them, the density profile) have been derived, a long time ago, by heuristic macroscopic arguments: one sum rule is about the asymptotic form along the wall of the truncated two-body density, the other one is about the dipole moment of the structure factor. In the two-dimensional case at $\beta e^2=2$, we have now explicit expressions up to order $\hbar^2$ of these two quantum densities, thus we can microscopically check the sum rules at this order. The checks are positive, reinforcing the idea that the sum rules are correct.
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PDF链接:
https://arxiv.org/pdf/704.2316