Canonical Quantization on a Doubly Connected Space and the Aharonov-Bohm Phase

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Abstract

We consider the canonical quantization (Schrödinger representation) on a doubly connected space ΩR≡R2\{(x, y)x2+y2≤R2} (R>0). We show that, when we employ 2-dimensional orthogonal coordinates Ox1x2, there are uncountably many different self-adjoint extensions pUj of pj≡-i∂/∂xj (j=1, 2), and none of the pairs {pj, qj′}j, j′=1, 2 (qj′≡xj′·) satisfies the Weyl relation. Then, we construct a new canonical pair of canonical momentum and position operators so that the pair can satisfy the Weyl relation by using the streamline coordinates. As its application, in the Weyl relation with respect to the pair of the mv-momentum and position operators by the above new canonical pair, we find the Aharonov-Bohm phase.

Original languageEnglish
Pages (from-to)322-363
Number of pages42
JournalJournal of Functional Analysis
Volume174
Issue number2
DOIs
Publication statusPublished - Jul 10 2000
Externally publishedYes

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Quantization
Momentum
Self-adjoint Extension
Streamlines
Operator

All Science Journal Classification (ASJC) codes

  • Analysis

Cite this

Canonical Quantization on a Doubly Connected Space and the Aharonov-Bohm Phase. / Hirokawa, Masao.

In: Journal of Functional Analysis, Vol. 174, No. 2, 10.07.2000, p. 322-363.

Research output: Contribution to journalArticle

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