Optical reflectivity and transmissivity of misfit layer compounds (MS)nTS2 (T = Ta, Nb; M = Pb, Sm, Tb; 1.08 < n < 1.23)

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  • C. H. Rüscher

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Original languageEnglish
Pages (from-to)889-904
Number of pages16
JournalPhysica Status Solidi (B) Basic Research
Volume198
Issue number2
Publication statusPublished - Dec 1996

Abstract

The room temperature transmission and reflection behaviour of misfit layer compounds (MLCs) (MS)nTS2 (T = Nb, Ta; M = Pb, Sm, Tb) were investigated in the spectral range between 1000 and 20000 cm-1 for incident light normal to the layered structure (k ⊥ (001)). A characteristic near infrared transmission window (TW) is observed between the Drude free carrier threshold (4000 cm-1 < w0 < 6000 cm-1) and the onset of stronger interband transitions (above 13000 cm-1). Evaluations of the absorption profiles show an interband absorption superimposed on the free carrier absorption in the TW which are related to transitions involving states in the conduction band (or conduction bands). Values of w0 are found to be slightly smaller for E ∥ b compared to E ∥ a (parallel to the incommensurate direction) polarized spectra for all compounds under study. This effect is interpreted in terms of slightly smaller effective masses for the optical conductivity for the E ∥ a components. The temperature dependence (213 to 423 K) of the free carrier reflectivity for (PbS)1.13TaS2 shows a linear increase of the damping parameter with temperature both for E ∥ a and E ∥ b. This is suggested to be due to ordinary electron-phonon scattering of the free carriers. Reflection spectra for E ∥ c indicate w0 values of about 1500 cm-1 for (SmS)1.19TaS2 ((TbS)1.21NbS2) and below 1300 cm-1 for (PbS)1.13TaS2 ((PbS)1.21NbS2).

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Optical reflectivity and transmissivity of misfit layer compounds (MS)nTS2 (T = Ta, Nb; M = Pb, Sm, Tb; 1.08 < n < 1.23). / Rüscher, C. H.
In: Physica Status Solidi (B) Basic Research, Vol. 198, No. 2, 12.1996, p. 889-904.

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abstract = "The room temperature transmission and reflection behaviour of misfit layer compounds (MLCs) (MS)nTS2 (T = Nb, Ta; M = Pb, Sm, Tb) were investigated in the spectral range between 1000 and 20000 cm-1 for incident light normal to the layered structure (k ⊥ (001)). A characteristic near infrared transmission window (TW) is observed between the Drude free carrier threshold (4000 cm-1 < w0 < 6000 cm-1) and the onset of stronger interband transitions (above 13000 cm-1). Evaluations of the absorption profiles show an interband absorption superimposed on the free carrier absorption in the TW which are related to transitions involving states in the conduction band (or conduction bands). Values of w0 are found to be slightly smaller for E ∥ b compared to E ∥ a (parallel to the incommensurate direction) polarized spectra for all compounds under study. This effect is interpreted in terms of slightly smaller effective masses for the optical conductivity for the E ∥ a components. The temperature dependence (213 to 423 K) of the free carrier reflectivity for (PbS)1.13TaS2 shows a linear increase of the damping parameter with temperature both for E ∥ a and E ∥ b. This is suggested to be due to ordinary electron-phonon scattering of the free carriers. Reflection spectra for E ∥ c indicate w0 values of about 1500 cm-1 for (SmS)1.19TaS2 ((TbS)1.21NbS2) and below 1300 cm-1 for (PbS)1.13TaS2 ((PbS)1.21NbS2).",
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AU - Rüscher, C. H.

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N2 - The room temperature transmission and reflection behaviour of misfit layer compounds (MLCs) (MS)nTS2 (T = Nb, Ta; M = Pb, Sm, Tb) were investigated in the spectral range between 1000 and 20000 cm-1 for incident light normal to the layered structure (k ⊥ (001)). A characteristic near infrared transmission window (TW) is observed between the Drude free carrier threshold (4000 cm-1 < w0 < 6000 cm-1) and the onset of stronger interband transitions (above 13000 cm-1). Evaluations of the absorption profiles show an interband absorption superimposed on the free carrier absorption in the TW which are related to transitions involving states in the conduction band (or conduction bands). Values of w0 are found to be slightly smaller for E ∥ b compared to E ∥ a (parallel to the incommensurate direction) polarized spectra for all compounds under study. This effect is interpreted in terms of slightly smaller effective masses for the optical conductivity for the E ∥ a components. The temperature dependence (213 to 423 K) of the free carrier reflectivity for (PbS)1.13TaS2 shows a linear increase of the damping parameter with temperature both for E ∥ a and E ∥ b. This is suggested to be due to ordinary electron-phonon scattering of the free carriers. Reflection spectra for E ∥ c indicate w0 values of about 1500 cm-1 for (SmS)1.19TaS2 ((TbS)1.21NbS2) and below 1300 cm-1 for (PbS)1.13TaS2 ((PbS)1.21NbS2).

AB - The room temperature transmission and reflection behaviour of misfit layer compounds (MLCs) (MS)nTS2 (T = Nb, Ta; M = Pb, Sm, Tb) were investigated in the spectral range between 1000 and 20000 cm-1 for incident light normal to the layered structure (k ⊥ (001)). A characteristic near infrared transmission window (TW) is observed between the Drude free carrier threshold (4000 cm-1 < w0 < 6000 cm-1) and the onset of stronger interband transitions (above 13000 cm-1). Evaluations of the absorption profiles show an interband absorption superimposed on the free carrier absorption in the TW which are related to transitions involving states in the conduction band (or conduction bands). Values of w0 are found to be slightly smaller for E ∥ b compared to E ∥ a (parallel to the incommensurate direction) polarized spectra for all compounds under study. This effect is interpreted in terms of slightly smaller effective masses for the optical conductivity for the E ∥ a components. The temperature dependence (213 to 423 K) of the free carrier reflectivity for (PbS)1.13TaS2 shows a linear increase of the damping parameter with temperature both for E ∥ a and E ∥ b. This is suggested to be due to ordinary electron-phonon scattering of the free carriers. Reflection spectra for E ∥ c indicate w0 values of about 1500 cm-1 for (SmS)1.19TaS2 ((TbS)1.21NbS2) and below 1300 cm-1 for (PbS)1.13TaS2 ((PbS)1.21NbS2).

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