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1
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85038302863
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For a review of early work on (formula presented) in high temperature superconductors, see, e.g., C. Uher, in, edited by D. M. Ginsberg (World Scientific, Singapore, 1992), 3
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For a review of early work on (formula presented) in high temperature superconductors, see, e.g., C. Uher, in Physical Properties of High Temperature Superconductors, edited by D. M. Ginsberg (World Scientific, Singapore, 1992), Vol. 3.
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2
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0000166047
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For more recent work on (formula presented) in high temperature superconductors see e.g., and
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85038289685
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In the superconducting state there also exists the so-called circulatory contribution (formula presented) to the heat current (see, e.g., Ref. It is given by (formula presented) where, is the thermopower and (formula presented) is the electrical resistivity. This contribution is usually very small. For example, in the high-(formula presented) superconductors (formula presented) (formula presented) and (formula presented) for (formula presented) close to optimum doping) we find (formula presented) much smaller than the experimental values (formula presented) found for single crystals
-
In the superconducting state there also exists the so-called circulatory contribution (formula presented) to the heat current (see, e.g., Ref. 1). It is given by (formula presented) where S is the thermopower and (formula presented) is the electrical resistivity. This contribution is usually very small. For example, in the high-(formula presented) superconductors (formula presented) (formula presented) and (formula presented) for (formula presented) close to optimum doping) we find (formula presented) much smaller than the experimental values (formula presented) found for single crystals.
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