Thermopower and thermal conductivity of superconducting perovskite MgCNi3
S. Y. Li, W. Q. Mo, M. Yu, W. H. Zheng, C. H. Wang, Y. M. Xiong, R. Fan, H. S. Yang, B. M. Wu, L. Z. Cao, X. H. Chen
DOI 10.1103/PhysRevB.65.064534 · Physical Review B
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Abstract
The thermopower and thermal conductivity of superconducting perovskite MgCNi3(Tc≈8 K) have been studied. The thermopower is negative from room temperature to 10 K. Combined with the negative Hall coefficient reported previously, the negative thermopower definitely indicates that the carrier in MgCNi3 is electron type. The nonlinear temperature dependence of thermopower below 150 K is explained by the electron-phonon interaction renormalization effects. The thermal conductivity is of the order for intermetallics, larger than that of borocarbides, and smaller than MgB2. In the normal state, the electronic contribution to the total thermal conductivity is slightly larger than the lattice contribution. The transverse magnetoresistance of MgCNi3 is also measured. It is found that the classical Kohler’s rule is valid above 50 K. An electronic crossover occurs at T*∼50 K, resulting in the abnormal behavior of resistivity, thermopower, and magnetoresistance below 50 K.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| MgCNi3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8 | Pressure not reported | midpoint |
| MgB2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 39 | Pressure not reported | unknown |
| LuNi2B2C Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 16 | Pressure not reported | unknown |
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