Abstract
It is widely held that the single most important parameter describing the strength of the electron-phonon interaction in superconductivity is the mass enhancement factor λ, and that the maximum possible transition temperature for a given class of materials (e.g., the polyvalent metals) is attained for a very large value, λ≈3, of the parameter. We show that it is not likely that the highest attainable values ofT c will reflect such large values of λ. Instead, we expect that they will be associated with values of λ that do not differ greatly from a value of about 1.5, and with very large values of the parameterA, whereA is the area under the electron-phonon interaction spectrum α2 F(v). This is certainly the case forNb 3 Sn, which has aT c of 18 K.
Similar content being viewed by others
References
G. M. Eliashberg,Soviet Phys.—JETP 11, 696 (1960).
D. J. Scalapino, inSuperconductivity, R. D. Parks, ed. (Marcel Dekker, New York, 1969).
W. L. McMillan and J. M. Rowell, inSuperconductivity, R. D. Parks, ed. (Marcel Dekker, New York, 1969).
W. L. McMillan,Phys. Rev. 167, 331 (1968).
R. C. Dynes,Solid State Commun. 10, 615 (1972).
L. Y. L. Shen,Phys. Rev. Lett. 29, 1082 (1972).
J. M. Rowell, W. L. McMillan, and R. C. Dynes, A tabulation of the electron-phonon interaction in superconducting metals and alloys (unpublished).
R. C. Dynes,Phys. Rev. B 2, 644 (1970).
Author information
Authors and Affiliations
Additional information
Research sponsored by the National Research Council of Canada.
Rights and permissions
About this article
Cite this article
Leavens, C.R., Carbotte, J.P. An important parameter in high-temperature superconductivity. J Low Temp Phys 14, 195–211 (1974). https://doi.org/10.1007/BF00654817
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF00654817