Photon Berry’s phase as a classical topological effect

Jan Segert
Phys. Rev. A 36, 10 – Published 1 July 1987
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Abstract

We discuss Berry’s phase rotation for electromagnetic radiation propagating in an optical fiber as a classical effect. We show that the evolution of the polarization vector is determined by a connection on the tangent bundle of the two-dimensional sphere. We use a topological argument to show that there exists only one rotationally invariant connection on the tangent bundle of the two sphere. The arguments apply to any classical transverse wave: for example, transverse vibrations propagating in a bent solid rod. The analogous effect in quantum electrodynamics, namely, Berry’s phase for a single photon propagating in an optical fiber, is a simple consequence of the classical effect described. We argue that this should be viewed as a classical, rather than a quantum, effect. We also comment on recent related work of Haldane and of Berry.

  • Received 19 December 1986

DOI:https://doi.org/10.1103/PhysRevA.36.10

©1987 American Physical Society

Authors & Affiliations

Jan Segert

  • Physics Department, Princeton University, Princeton, New Jersey 08544

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Vol. 36, Iss. 1 — July 1987

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