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대한전자공학회 워크샵

On A Mathematical Theory of Quantization

Hiroyasu Koshimizu

Published Feb 1, 2003• 0 citations
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Luther Rinehart

The formulation of classical mechanics applicable to fermionic degrees of freedom is presented in mathematically rigorous terms, including a description of how the mathematical structure relates to the quantization of the theory. Canonical transformations and the algebra of observables are defined and studied. A formula is given for the analog of the Poisson bracket. The quantization of the theory proceeds according to deformation quantization.

arXiv:1505.00237•May 1, 2015•0 citations

From Weyl quantization to modern algebraic index theory

Markus J. Pflaum

Introduction One of the most influencial contributions of H ermann W eyl to mathematical physics has been his paper Gruppentheorie und Quantenmechanik [W e 27] from 1927 and its extended version, the book [W e 28] which was published a year later and carries the same title. The main topic of this part of H ermann W eyl's work is the mathematics of quantum mechanics. After the fundamental papers by H eisenberg and S chrödinger on the foundations of quantum mechanics had appeared in the twenties of the last century this was the central question studied in mathematical physics at that time and which to a certain degree still is present in all attempts to construct mathematically rigorous theories unifying quantum mechanics and general realtivity. In his article Gruppentheorie und Quantenmechanik , H ermann W eyl essentially introduced two novel aspects to the mathematics of quantum mechanics, namely the following: (i) The representation theory of (compact) Lie groups on Hilbert spaces was applied to mathematically determine atomic spectra. (ii) A conceptually clear quantization method was proposed which associates quantum mechanical operators to classical observables which mathematically are represented by appropriate functions of the space and momentum variables. Nowadays, this quantization scheme is named after his inventor Weyl quantization. In this paper I will elaborate only on the second aspect, since the representation theory of compact Lie groups has already been covered in detail in other contributions to these proceedings.

Cambridge University Press eBooks•Oct 16, 2008•0 citations

On the Method of Second Quantization

Richard Becker, G�nther Leibfried

Physical Review•Jan 1, 1946•24 citations
Introduction One of the most influencial contributions of H ermann W eyl to mathematical physics has been his paper Gruppentheorie und Quantenmechanik [W e 27] from 1927 and its extended version, the book [W e 28] which was published a year later and carries the same title. The main topic of this part of H ermann W eyl's work is the mathematics of quantum mechanics. After the fundamental papers by H eisenberg and S chrödinger on the foundations of quantum mechanics had appeared in the twenties of the last century this was the central question studied in mathematical physics at that time and which to a certain degree still is present in all attempts to construct mathematically rigorous theories unifying quantum mechanics and general realtivity. In his article Gruppentheorie und Quantenmechanik , H ermann W eyl essentially introduced two novel aspects to the mathematics of quantum mechanics, namely the following: (i) The representation theory of (compact) Lie groups on Hilbert spaces was applied to mathematically determine atomic spectra. (ii) A conceptually clear quantization method was proposed which associates quantum mechanical operators to classical observables which mathematically are represented by appropriate functions of the space and momentum variables. Nowadays, this quantization scheme is named after his inventor Weyl quantization. In this paper I will elaborate only on the second aspect, since the representation theory of compact Lie groups has already been covered in detail in other contributions to these proceedings.