Abstract

We present a classical linear response theory for a magneto–dielectric material and determine the polariton dispersion relations. The electromagnetic field fluctuation spectra are obtained and polariton sum rules for their optical parameters are presented. The electromagnetic field for systems with multiple polariton branches is quantized in three dimensions and field operators are converted to 1–dimensional forms appropriate for parallel light beams. We show that the field–operator commutation relations agree with previous calculations that ignored polariton effects. The Abraham (kinetic) and Minkowski (canonical) momentum operators are introduced and their corresponding single–photon momenta are identified. The commutation relations of these and of their angular analogues support the identification, in particular, of the Minkowski momentum with the canonical momentum of the light. We exploit the Heaviside–Larmor symmetry of Maxwell’s equations to obtain, very directly, the Einsetin–Laub force density for action on a magneto–dielectric. The surface and bulk contributions to the radiation pressure are calculated for the passage of an optical pulse into a semi–infinite sample.

Highlights

  • At the heart of the problem of radiation pressure is the famous Abraham–Minkowski dilemma concerning the correct form of the electromagnetic momentum in a material medium [1,2,3,4]; a problem which, despite of its longevity, continues to attract attention [5,6,7,8,9]

  • In this paper we shall be concerned with manifestations of optical momentum in radiation pressure on media and, in particular, on magneto–dielectric media

  • We shall make use of the 1D field operators derived here to calculate the force exerted by a photon on a magneto–dielectric medium, but first return to the full 3D description to investigate the electromagnetic momentum

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Summary

Introduction

At the heart of the problem of radiation pressure is the famous Abraham–Minkowski dilemma concerning the correct form of the electromagnetic momentum in a material medium [1,2,3,4]; a problem which, despite of its longevity, continues to attract attention [5,6,7,8,9]. The resolution of this dilemma lies is the identification of the two momenta, due to Abraham and Minkowski, with the kinetic and canonical momenta of the light, respectively [10]. S M Barnett and R Loudon transfer from light to a half–space sample and so provide the extension to permeable media of earlier work on dielectrics [18]

Classical theory
Field fluctuations
Quantum theory
Parallel beams
Momentum operators
Magnetic Lorentz force
Conclusion
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