2008
DOI: 10.1070/rc2008v077n01abeh003746
|View full text |Cite
|
Sign up to set email alerts
|

Chemical aspects of the design of thermoelectric materials

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4

Citation Types

1
70
0
5

Year Published

2008
2008
2014
2014

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 140 publications
(81 citation statements)
references
References 130 publications
(136 reference statements)
1
70
0
5
Order By: Relevance
“…14 Ta-doped SrTiO 3 might also be a good or even better TE material, since Ta doping compared with Nb doping will result in the intensification of the phonon scattering and, correspondingly, the reduction of the lattice thermal conductivity. 15 We have successfully doped Ta into SrTiO 3 samples, and a series of samples have been characterized by powder x-ray diffraction and EPMA.…”
Section: Introductionmentioning
confidence: 99%
“…14 Ta-doped SrTiO 3 might also be a good or even better TE material, since Ta doping compared with Nb doping will result in the intensification of the phonon scattering and, correspondingly, the reduction of the lattice thermal conductivity. 15 We have successfully doped Ta into SrTiO 3 samples, and a series of samples have been characterized by powder x-ray diffraction and EPMA.…”
Section: Introductionmentioning
confidence: 99%
“…These compounds have attracted attention only during the last two decades as a result of the development of the "phonon glass-electron crystal" concept, [2] according to which inorganic clathrates are considered as prospective thermoelectric materials (TMs). [3][4][5] The possibility of varying their thermal and electric transport properties independently arises directly from their structure features, being a necessary condition for an efficient TM. [4][5][6] High thermoelectric efficiency (ZT) has been observed for the clathrates Sr 8 Ge 30 Ga 16 (ZT % 0.25 at T = 300 K) and Ba 8 Ge 30 Ga 16 (ZT > 1 at T > 800 K).…”
Section: Introductionmentioning
confidence: 99%
“…In ideal thermoelectric materials, a high electrical conductivity (s) needs to be combined with a high Seebeck coefficient (S) and a low total thermal conductivity (k). [6,7,8] However, as all of these properties depend on the charge-carrier concentration, they cannot be varied independently. The efficiencies of thermoelectric generators depend on the dimensionless figure of merit, ZT = S 2 sTk…”
Section: Introductionmentioning
confidence: 99%