2005
DOI: 10.1016/j.jpcs.2005.05.077
|View full text |Cite
|
Sign up to set email alerts
|

Temperature dependence of thermoelectric properties of Ni-doped CoSb3

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

3
41
1

Year Published

2010
2010
2022
2022

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 75 publications
(45 citation statements)
references
References 3 publications
3
41
1
Order By: Relevance
“…15 Very recently, CoSb 3 filled with electronegative atoms (S and Se) were successfully prepared with a strong covalent guest-host interactions between S (or Se) and Sb, which leads to very low lattice thermal conductivity. 17 The second approach is substituting Co or Sb atoms with metals or semimetals to tune the electronic properties, [17][18][19][20][21][22][23] and lots of experimental studies show VIA-group element (O, S, Se, Te) dopants can significantly influence the TE properties of CoSb 3 . 17,18,[24][25][26][27] For Te doped CoSb 3 , Te substituting Sb (Te Sb ) would be the dominant point defect.…”
Section: Zt T α σ κ =mentioning
confidence: 99%
See 1 more Smart Citation
“…15 Very recently, CoSb 3 filled with electronegative atoms (S and Se) were successfully prepared with a strong covalent guest-host interactions between S (or Se) and Sb, which leads to very low lattice thermal conductivity. 17 The second approach is substituting Co or Sb atoms with metals or semimetals to tune the electronic properties, [17][18][19][20][21][22][23] and lots of experimental studies show VIA-group element (O, S, Se, Te) dopants can significantly influence the TE properties of CoSb 3 . 17,18,[24][25][26][27] For Te doped CoSb 3 , Te substituting Sb (Te Sb ) would be the dominant point defect.…”
Section: Zt T α σ κ =mentioning
confidence: 99%
“…is the density of states of ideal host cell, and is the Fermi-Dirac distribution given by: 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 13 (8) Following the procedure described above, the Fermi level (E F ) and free carriers can be determined by iteratively solving the overall charge neutrality requirement, as displayed in 17 The annealing temperature region of CoSb 3 is generally around 850 -1100 K. [14][15][16][17][18][19][20][21][22][23] The electron carrier concentration is found to be The total composition x of a phase with defects within an equilibrium set of atomic chemical potentials can be calculated by:…”
Section: Defect Carrier Concentration and Solubility Limitation In M mentioning
confidence: 99%
“…[13][14][15][16][17] Those phonons are primarily scattered by features in the structure (dopant, nanostructures and so on) that are comparable in size to the MFP of the phonons. For example, the high-frequency (short-wavelength) phonons tend to be scattered more effectively by atomic-scale point defects, that is, doping foreign species at the sites of Co 18,19 and Sb 7,11,20,21 or introducing filler atoms [22][23][24] into the structural voids (cages) of CoSb 3 . The medium-frequency phonons with medium MFP of several to hundreds of nanometers are significantly scattered by nanoprecipitates or other nanoscale heterogeneities.…”
Section: Introductionmentioning
confidence: 99%
“…However, these elements have filling limitations. 7 Doping of partial Co [8][9][10] or Sb-site [11][12][13] substitution has also been widely studied to lower the thermal conductivity through phonon scattering on impurities.…”
Section: Introductionmentioning
confidence: 99%