The Contribution of Phonons to the Thomson Coefficient
Keyword(s):
An electric current of density j flowing in a temperature gradient \1T gives up heat in a reversible way; the amount of heat thus liberated per unit volume and unit time is given by -p.j\1T, (1) p. being the Thomson coefficient, which can be shown to be T d r l(Kl )' p.=-e dT(P Ko -~ 5' (2) where ~ is the Fermi energy, and the K's are the usual transport coefficients as defined by Mott and Jones (1936, p. 306, equation (99)), or more generally by Wilson (1953, p. 305).
1994 ◽
Vol 52
(2)
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pp. 309-319
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1993 ◽
Vol 50
(1)
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pp. 125-144
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2013 ◽
Vol 740-742
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pp. 3-6
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2008 ◽
Vol 22
(01n02)
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pp. 120-120
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2019 ◽
Vol 45
(17)
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pp. 22987-22990
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2012 ◽
Vol 535
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pp. 182-188
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