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Classical Limit on Quantum Mechanics for Unbounded Observables.

机译:无界可观测物的量子力学经典极限。

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摘要

This dissertation is divided into two parts. In Part I of this dissertation--- On the Classical Limit of Quantum Mechanics, we extend a method introduced by Hepp in 1974 for studying the asymptotic behavior of quantum expectations in the limit as Plank's constant (h) tends to zero. The goal is to allow for unbounded observables which are (non-commutative) polynomial functions of the position and momentum operators. [This is in contrast to Hepp's original paper where the "observables" were, roughly speaking, required to be bounded functions of the position and momentum operators.] As expected the leading order contributions of the quantum expectations come from evaluating the "symbols" of the observables along the classical trajectories while the next order contributions (quantum corrections) are computed by evolving the h=1 observables by a linear canonical transformations which is determined by the second order pieces of the quantum mechanical Hamiltonian.;Part II of the dissertation --- Powers of Symmetric Differential Operators is devoted to operator theoretic properties of a class of linear symmetric differential operators on the real line. In more detail, let L and L˜ be a linear symmetric differential operator with polynomial coefficients on L2 (m) whose domain is the Schwartz test function space, S. We study conditions on the polynomial coefficients of L and L˜ which implies operator comparison inequalities of the form (L˜+C˜r ≤ Cr (L¯+C) r for all 0 ≤ r < infinity. These comparison inequalities (along with their generalizations allowing for the parameter h>0 in the coefficients) are used to supply a large class of Hamiltonian operators which verify the assumptions needed for the results in Part I of this dissertation.
机译:本文分为两个部分。在本论文的第一部分-关于量子力学的经典极限,我们扩展了Hepp于1974年引入的一种方法,用于研究当Plank常数(h)趋于零时极限中的量子期望的渐近行为。目的是允许无限制的可观测量,它们是位置和动量算子的(非交换)多项式函数。 [这与Hepp的原始论文形成对比,在粗略地说,“可观察物”被要求是位置和动量算子的有界函数。]正如所期望的那样,量子期望的前导贡献来自于估计的“符号”。沿经典轨迹的可观测量,而下一阶贡献(量子校正)是通过将h = 1可观测量通过线性经典变换演化而来计算的,该线性正则变换由量子力学哈密顿量的二阶确定。;论文的第二部分- -对称微分算子的幂致力于实线上一类线性对称微分算子的算子理论性质。更详细地讲,令L和L〜为线性对称对称微分算子,其域为Schwartz检验函数空间S为L2(m)上的多项式系数。我们研究L和L〜的多项式系数的条件,这意味着算符比较对于所有0≤r <无穷大,形式为(L〜+ C〜r≤Cr(L'+ C)r的形式的不等式。这些比较式不等式(以及它们的泛化允许系数h> 0)用于:提供了一大类哈密顿算子,这些算子验证了本文第一部分结果所需要的假设。

著录项

  • 作者

    Tong, Pun Wai.;

  • 作者单位

    University of California, San Diego.;

  • 授予单位 University of California, San Diego.;
  • 学科 Mathematics.
  • 学位 Ph.D.
  • 年度 2016
  • 页码 214 p.
  • 总页数 214
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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