Volume 127, Issue 1 pp. 187-200

Original Paper

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General Theory of Secondary Radiation in Condensed Matter

I. G. Lang,

I. G. Lang

A. F. Ioffe Physico-Technical Institute, Academy of Sciences of the USSR, Leningrad

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S. T. Pavlov,

S. T. Pavlov

A. F. Ioffe Physico-Technical Institute, Academy of Sciences of the USSR, Leningrad

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A. V. Prokaznikov,

A. V. Prokaznikov

A. F. Ioffe Physico-Technical Institute, Academy of Sciences of the USSR, Leningrad

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A. V. Goltsev,

A. V. Goltsev

A. F. Ioffe Physico-Technical Institute, Academy of Sciences of the USSR, Leningrad

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I. G. Lang,

I. G. Lang

A. F. Ioffe Physico-Technical Institute, Academy of Sciences of the USSR, Leningrad

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S. T. Pavlov,

S. T. Pavlov

A. F. Ioffe Physico-Technical Institute, Academy of Sciences of the USSR, Leningrad

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A. V. Prokaznikov,

A. V. Prokaznikov

A. F. Ioffe Physico-Technical Institute, Academy of Sciences of the USSR, Leningrad

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A. V. Goltsev,

A. V. Goltsev

A. F. Ioffe Physico-Technical Institute, Academy of Sciences of the USSR, Leningrad

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First published: 1 January 1985

https://doi.org/10.1002/pssb.2221270118

Citations: 4

194021 Leningrad, USSR.

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Abstract

A general theory is given accounting for the secondary radiation which is excited in condensed matter exposed by light at finite temperatures, T ≧ ħω_s, where ω_s is the radiation frequency. The formula which is derived for a light scattering tensor of rank four, is similar to that obtained by Kubo for the conductivity tensor. It allows for all types of interactions possible within the scattering medium. The obtained results are compared to conclusions in the cases of either low, T ≪ ħω_s, or T ≥ ħω_s temperatures.

Abstract

Es wird eine allgemeine Theorie für die Sekundaärstrahlung vorgestellt, die in kondensierter Materie, die bei endlichen Temperaturen, T ≧ ħω_s, mit Licht bestrahlt wird, wobei ω_s die Strahlungsfrequenz ist, angeregt wird. Die Formel, die für einen Lichtstreutensor vom Rang vier abgeleitet wird, ist der, die von Kubo für den Leitfähigkeitstensor erhalten wird, ähnlich. Sie gilt für alle Wechselwirkungen, die im streuenden Medium möglich sind. Die erhaltenen Ergebnisse werden mit früheren Schlußfolgerungen im Falle von entweder tiefen, T ≪ ħω_s, oder hohen, T ≧ ħω_s, Temperaturen verglichen.

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Volume127, Issue1

1 January 1985

Pages 187-200

General Theory of Secondary Radiation in Condensed Matter

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General Theory of Secondary Radiation in Condensed Matter

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