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Volumn 5, Issue 2, 2012, Pages 5510-5530

Resonant levels in bulk thermoelectric semiconductors

Author keywords

[No Author keywords available]

Indexed keywords

BAND STRUCTURE ENGINEERING; COMPOUND SEMICONDUCTORS; CRYOGENIC TEMPERATURES; DELOCALIZATIONS; DENSITY OF STATE; ELECTRON ENERGIES; ELECTRONIC DENSITY; ELECTRONIC STRUCTURE CALCULATIONS; HYBRIDIZATION EFFECTS; IMPURITY LEVEL; IMPURITY STATE; POTENT MECHANISM; POWER FACTORS; RESONANT LEVELS; RESONANT SCATTERING; STRONGLY CORRELATED ELECTRON SYSTEM; THERMOELECTRIC SEMICONDUCTOR; THERMOPOWER ENHANCEMENT;

EID: 84856756898     PISSN: 17545692     EISSN: 17545706     Source Type: Journal    
DOI: 10.1039/c1ee02612g     Document Type: Review
Times cited : (821)

References (143)
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  • 15
    • 77956957276 scopus 로고    scopus 로고
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    • 3 is anisotropic in general, but the partial thermopowers of each electron or hole pocket of the Fermi surface are scalars. The anisotropy arises from the fact that the total thermopower is an average of the partial coefficients of each pocket weighted by the partial conductivities of those pockets, which are anisotropic. In degenerately-doped material, all pockets are degenerate, and the thermopower equals the partial hole thermopower of a pocket
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.