Thermal conductivity of CuGaTe"2
The thermal conductivity data of CuGaTe"2, measured at low temperatures, are analyzed by using the full Callaway expression for an isotropic model. It is observed that the predominant scattering of phonons in this temperature range is due to extended defects or clusters. This confirms earlier s...
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1987 |
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| Reproduktion: |
Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
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| Übergeordnetes Werk: |
in: Solid State Communications - Amsterdam : Elsevier, 64(1987), 4, Seite 439-442 |
| Übergeordnetes Werk: |
volume:64 ; year:1987 ; number:4 ; pages:439-442 |
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| 520 | |a The thermal conductivity data of CuGaTe"2, measured at low temperatures, are analyzed by using the full Callaway expression for an isotropic model. It is observed that the predominant scattering of phonons in this temperature range is due to extended defects or clusters. This confirms earlier suggestions of the possible existence of a second phase in this compound grown from stoichiometric compositions. It is estimated that the average radius and the concentration of these defects are 18^oA and 6.6 x 10^1^6 cm^-^3, respectively. | ||
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(DE-627)NLEJ178546275 (DE-599)GBVNLZ178546275 DE-627 ger DE-627 rakwb eng Thermal conductivity of CuGaTe"2 1987 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The thermal conductivity data of CuGaTe"2, measured at low temperatures, are analyzed by using the full Callaway expression for an isotropic model. It is observed that the predominant scattering of phonons in this temperature range is due to extended defects or clusters. This confirms earlier suggestions of the possible existence of a second phase in this compound grown from stoichiometric compositions. It is estimated that the average radius and the concentration of these defects are 18^oA and 6.6 x 10^1^6 cm^-^3, respectively. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Wasim, S.M. oth Noguera, A. oth in Solid State Communications Amsterdam : Elsevier 64(1987), 4, Seite 439-442 (DE-627)NLEJ176858040 (DE-600)1467698-9 0038-1098 nnns volume:64 year:1987 number:4 pages:439-442 http://linkinghub.elsevier.com/retrieve/pii/0038-1098(87)90754-X GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 64 1987 4 439-442 |
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(DE-627)NLEJ178546275 (DE-599)GBVNLZ178546275 DE-627 ger DE-627 rakwb eng Thermal conductivity of CuGaTe"2 1987 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The thermal conductivity data of CuGaTe"2, measured at low temperatures, are analyzed by using the full Callaway expression for an isotropic model. It is observed that the predominant scattering of phonons in this temperature range is due to extended defects or clusters. This confirms earlier suggestions of the possible existence of a second phase in this compound grown from stoichiometric compositions. It is estimated that the average radius and the concentration of these defects are 18^oA and 6.6 x 10^1^6 cm^-^3, respectively. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Wasim, S.M. oth Noguera, A. oth in Solid State Communications Amsterdam : Elsevier 64(1987), 4, Seite 439-442 (DE-627)NLEJ176858040 (DE-600)1467698-9 0038-1098 nnns volume:64 year:1987 number:4 pages:439-442 http://linkinghub.elsevier.com/retrieve/pii/0038-1098(87)90754-X GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 64 1987 4 439-442 |
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(DE-627)NLEJ178546275 (DE-599)GBVNLZ178546275 DE-627 ger DE-627 rakwb eng Thermal conductivity of CuGaTe"2 1987 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The thermal conductivity data of CuGaTe"2, measured at low temperatures, are analyzed by using the full Callaway expression for an isotropic model. It is observed that the predominant scattering of phonons in this temperature range is due to extended defects or clusters. This confirms earlier suggestions of the possible existence of a second phase in this compound grown from stoichiometric compositions. It is estimated that the average radius and the concentration of these defects are 18^oA and 6.6 x 10^1^6 cm^-^3, respectively. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Wasim, S.M. oth Noguera, A. oth in Solid State Communications Amsterdam : Elsevier 64(1987), 4, Seite 439-442 (DE-627)NLEJ176858040 (DE-600)1467698-9 0038-1098 nnns volume:64 year:1987 number:4 pages:439-442 http://linkinghub.elsevier.com/retrieve/pii/0038-1098(87)90754-X GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 64 1987 4 439-442 |
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(DE-627)NLEJ178546275 (DE-599)GBVNLZ178546275 DE-627 ger DE-627 rakwb eng Thermal conductivity of CuGaTe"2 1987 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The thermal conductivity data of CuGaTe"2, measured at low temperatures, are analyzed by using the full Callaway expression for an isotropic model. It is observed that the predominant scattering of phonons in this temperature range is due to extended defects or clusters. This confirms earlier suggestions of the possible existence of a second phase in this compound grown from stoichiometric compositions. It is estimated that the average radius and the concentration of these defects are 18^oA and 6.6 x 10^1^6 cm^-^3, respectively. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Wasim, S.M. oth Noguera, A. oth in Solid State Communications Amsterdam : Elsevier 64(1987), 4, Seite 439-442 (DE-627)NLEJ176858040 (DE-600)1467698-9 0038-1098 nnns volume:64 year:1987 number:4 pages:439-442 http://linkinghub.elsevier.com/retrieve/pii/0038-1098(87)90754-X GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 64 1987 4 439-442 |
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(DE-627)NLEJ178546275 (DE-599)GBVNLZ178546275 DE-627 ger DE-627 rakwb eng Thermal conductivity of CuGaTe"2 1987 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The thermal conductivity data of CuGaTe"2, measured at low temperatures, are analyzed by using the full Callaway expression for an isotropic model. It is observed that the predominant scattering of phonons in this temperature range is due to extended defects or clusters. This confirms earlier suggestions of the possible existence of a second phase in this compound grown from stoichiometric compositions. It is estimated that the average radius and the concentration of these defects are 18^oA and 6.6 x 10^1^6 cm^-^3, respectively. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Wasim, S.M. oth Noguera, A. oth in Solid State Communications Amsterdam : Elsevier 64(1987), 4, Seite 439-442 (DE-627)NLEJ176858040 (DE-600)1467698-9 0038-1098 nnns volume:64 year:1987 number:4 pages:439-442 http://linkinghub.elsevier.com/retrieve/pii/0038-1098(87)90754-X GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 64 1987 4 439-442 |
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The thermal conductivity data of CuGaTe"2, measured at low temperatures, are analyzed by using the full Callaway expression for an isotropic model. It is observed that the predominant scattering of phonons in this temperature range is due to extended defects or clusters. This confirms earlier suggestions of the possible existence of a second phase in this compound grown from stoichiometric compositions. It is estimated that the average radius and the concentration of these defects are 18^oA and 6.6 x 10^1^6 cm^-^3, respectively. |
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The thermal conductivity data of CuGaTe"2, measured at low temperatures, are analyzed by using the full Callaway expression for an isotropic model. It is observed that the predominant scattering of phonons in this temperature range is due to extended defects or clusters. This confirms earlier suggestions of the possible existence of a second phase in this compound grown from stoichiometric compositions. It is estimated that the average radius and the concentration of these defects are 18^oA and 6.6 x 10^1^6 cm^-^3, respectively. |
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The thermal conductivity data of CuGaTe"2, measured at low temperatures, are analyzed by using the full Callaway expression for an isotropic model. It is observed that the predominant scattering of phonons in this temperature range is due to extended defects or clusters. This confirms earlier suggestions of the possible existence of a second phase in this compound grown from stoichiometric compositions. It is estimated that the average radius and the concentration of these defects are 18^oA and 6.6 x 10^1^6 cm^-^3, respectively. |
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