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Specific features of the optical absorption edge anisotropy in In4(P2S6)3 layered crystals

Identifieur interne : 00EA26 ( Main/Repository ); précédent : 00EA25; suivant : 00EA27

Specific features of the optical absorption edge anisotropy in In4(P2S6)3 layered crystals

Auteurs : RBID : Pascal:03-0118423

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Abstract

The optical absorption edge of In4(P2S6)3 layered crystals is studied in the temperature range 77-355 K. In the spectral range of direct optical transitions, the absorption edge is of Urbach shape. Electron-phonon interaction result in the smearing of energy bands and, consequently, in appearing of Urbach absorption tails. The temperature variation of the optical pseudogap E*g and the absorption edge energy width w are well described in the Einstein model. Strong anisotropy of the absorption edge spectral position and shape, as well as of electron-phonon interaction, is revealed.

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Pascal:03-0118423

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<title xml:lang="en" level="a">Specific features of the optical absorption edge anisotropy in In
<sub>4</sub>
(P
<sub>2</sub>
S
<sub>6</sub>
)
<sub>3</sub>
layered crystals</title>
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<name sortKey="Kranjcec, M" uniqKey="Kranjcec M">M. Kranjcec</name>
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<term>Indium Thiophosphates</term>
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<div type="abstract" xml:lang="en">The optical absorption edge of In
<sub>4</sub>
(P
<sub>2</sub>
S
<sub>6</sub>
)
<sub>3</sub>
layered crystals is studied in the temperature range 77-355 K. In the spectral range of direct optical transitions, the absorption edge is of Urbach shape. Electron-phonon interaction result in the smearing of energy bands and, consequently, in appearing of Urbach absorption tails. The temperature variation of the optical pseudogap E*
<sub>g</sub>
and the absorption edge energy width w are well described in the Einstein model. Strong anisotropy of the absorption edge spectral position and shape, as well as of electron-phonon interaction, is revealed.</div>
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<sub>4</sub>
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<sub>2</sub>
S
<sub>6</sub>
)
<sub>3</sub>
layered crystals is studied in the temperature range 77-355 K. In the spectral range of direct optical transitions, the absorption edge is of Urbach shape. Electron-phonon interaction result in the smearing of energy bands and, consequently, in appearing of Urbach absorption tails. The temperature variation of the optical pseudogap E*
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