Superconducting critical temperature and the isotope exponent versus total electron concentration for two-band superconductors: Effect of the band structure
J. J. Rodríguez-Núñez, A. A. Schmidt
DOI 10.1103/PhysRevB.68.224512 · Physical Review B
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Abstract
We consider the superconducting critical temperature Tc and the isotope exponent α versus carrier concentration ρ using the one-particle Green functions of the simplest coupled Hamiltonian for the two-band model with a single Tc [N. Kristoffel and P. Rubin, Physica C 356, 171 (2001)]. One of the bands, ɛ2(k→), is taken to be two dimensional, while the second band ɛ3(k→) is taken to be three dimensional. Taking only nearest-neighbor hopping for each one of the bands, we obtain that Tc versus ρ is symmetric around half filling in agreement with a general theorem of quantum mechanics. We also obtained the chemical potential μ versus ρ for several values of attractive interaction. We find that (1) the superconducting critical temperature Tc is maximum at ρ=1/2; (2) the chemical potential remains basically inside the smaller band, for the range of carrier concentration and Debye frequencies considered; (3) the isotope exponent has several symmetric minima around half filling depending on the anisotropy of the three-dimensional tight-binding band, namely, γ≡t3,x/t3,z≠1; (4) the chemical-potential curves, namely, μ versus ρ are completely independent of pairing interaction and Debye frequency; and (5) the number of symmetric minima and Tcmax goes down with increasing t3/t2 ratio. We have briefly discussed the possible relevance of our results with recent experimental data of the two-band compound MgB2.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| 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. | — | Pressure not reported | unknown |
| YNi2B2C Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Sr2RuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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