1995
DOI: 10.1103/physreva.52.1538
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Electromagnetic-field quantization in inhomogeneous and dispersive one-dimensional systems

Abstract: The electromagnetic field is quantized in a material whose dielectric function varies with frequency and one spatial dimension. The dielectric function is assumed to have a known form and to be real over the range of frequencies important for a particular application, for example the propagation of an optical signal. General properties of the mode functions are derived and employed in the quantization procedure. Expressions are obtained for the energy and momentum density and current operators, and these are s… Show more

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Cited by 51 publications
(36 citation statements)
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“…17 One method is to set \ 0 t1&cos(/)Ân, and then to split the inner integral at \=1&1Ân 1Â2 , approximating the two parts separately. The end result reads…”
Section: Appendix C: the Phase-space Volumes 8 Ijmentioning
confidence: 99%
See 1 more Smart Citation
“…17 One method is to set \ 0 t1&cos(/)Ân, and then to split the inner integral at \=1&1Ân 1Â2 , approximating the two parts separately. The end result reads…”
Section: Appendix C: the Phase-space Volumes 8 Ijmentioning
confidence: 99%
“…Although quantum theories of the electromagnetic field in such materials are developing rapidly (see e.g. [17], [14], [8], [9]), they are still some way short of affording descriptions of MIR, especially in 3D. Meanwhile our own experience discourages speculation: only with great trepidation do we mention even the most plausible of conjectures, that in a material modelled as a plasma, harmonic oscillations with 0<| p should not radiate into the interior, simply because a plasma (unlike our nondispersive model) has no propagating modes below | p at all.…”
Section: Summary Comments and Open Questionsmentioning
confidence: 99%
“…The same notion of one-dimensional Fox-Li mode is also implicit in an earlier paper by Lugiato and Narducci [52]. In this section, we will show how one-dimensional Fox-Li modes can be derived in the same rigorous way as normal modes are derived: from a Sturm-Liouville treatment [32,53]. For normal modes, perfect cavity boundary conditions are applied.…”
Section: Fox-li Modes As Natural Modesmentioning
confidence: 97%
“…Quantization of the electromagnetic field in dielectrics with real and frequency-independent permittivity has been treated extensively [1,2,3,4,5,6,7,8,9,10,11,12,13]. In the same context, dispersive dielectrics have been considered [14,15,16,17,18,19,20]. However, it is well known that the permittivity is a complex function of frequency which has to satisfy the Kramers-Kronig relations which state that the real part of the permittivity (responsible for dispersion) and the imaginary part (responsible for absorption) are necessarily connected with each other.…”
Section: Introductionmentioning
confidence: 99%