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The Particle Structure of the Quantum Mechanical Bose and Fermi Gas

机译:量子机械玻色和费米气体的粒子结构

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In the framework of von Neumann's description of measurements of discrete quantum observables we establish a one-to-one correspondence between symmetric statistical operators W of quantum mechanical systems and classical point processes kappa(W), thereby giving a particle picture of indistinguishable quantum particles. This holds true under irreducibility assumptions if we fix the underlying complete orthonormal system. The method of the Campbell measure is developed for such statistical operators; it is shown that the Campbell measure of a statistical operator W coincides with the Campbell measure of the corresponding point process kappa(W). Moreover, again under irreducibility assumptions, a symmetric statistical operator is completely determined by its Campbell measure. Themethod of the Campbell measure then is used to characterize Bose-Einstein and Fermi-Dirac statistical operators. This is an elementary introduction into the work of Fichtner and Freudenberg [10, 11] combined with the quantum mechanical investigations of [2] and the corresponding point process approach of [30]. It is based on the classical work of von Neumann [22], Segal, Cook and Chaiken [7, 8, 28] as well as Moyal [18].
机译:在冯·诺伊曼(von Neumann)的离散量子可观测量的描述框架中,我们建立了量子力学系统的对称统计算子W与经典点过程kappa(W)的一一对应关系,从而给出了不可区分的量子粒子的粒子图像。如果我们修复基础完整的正交系统,则在不可约性假设下也是如此。坎贝尔测度的方法是为此类统计运算符开发的;结果表明,统计算子W的坎贝尔度量与相应点过程kappa(W)的坎贝尔度量一致。此外,再次在不可约性假设下,对称统计算子完全由其Campbell度量确定。然后,使用Campbell度量方法来表征Bose-Einstein和Fermi-Dirac统计算子。这是对Fichtner和Freudenberg [10,11]的工作的基本介绍,结合了[2]的量子力学研究和[30]的相应点过程方法。它基于冯·诺依曼[22],西格尔,库克和柴肯[7、8、28]以及莫亚尔[18]的经典著作。

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