TY - JOUR
T1 - Calculation of λ for the quasi-one-dimensional superconductor V3Si
AU - Entin-Wohlman, O.
AU - Weger, W.
N1 - Funding Information:
This work was supported by a grant from the National Council for Research and Development, Israel and KFK (Kernforschungszentrum, Karlsruhe, Germany).
PY - 1983
Y1 - 1983
N2 - The band structure and the electron-phonon coupling are calculated for a σ-band hybridized with a δ1-band using tight-binding parameters fit for V3Si. The hybridization gives rise to a sharp peak in the electronic density of states near the state Γ12 of the δ1-band. The variation of the parameter N(0)I2 (N(0) - the electronic density of states at the Fermi level, I2 - the electron-phonon coupling constant) is studied at the vicinity of the Γ12(δ1) peak. It is found that there is some compensation between N(0) and I2; the narrow δ1-band gives rise to a large value of N(0), but a small value of I2; while the σ-band gives rise to a large value of I2, but a small value of N(0). As a result, the product N(0)I2 does not follow the behavior of N(0) even qualitatively, and it possesses a maximum far from the peak in N(0). Following this calculation, and previous calculations for the δ2 and σ-bands, an approximate relationship is developed for the contribution λito λ, coming from the various sub-bands of the 3d band, depending on the individual width of the sub-band, and its contribution to the density of states.
AB - The band structure and the electron-phonon coupling are calculated for a σ-band hybridized with a δ1-band using tight-binding parameters fit for V3Si. The hybridization gives rise to a sharp peak in the electronic density of states near the state Γ12 of the δ1-band. The variation of the parameter N(0)I2 (N(0) - the electronic density of states at the Fermi level, I2 - the electron-phonon coupling constant) is studied at the vicinity of the Γ12(δ1) peak. It is found that there is some compensation between N(0) and I2; the narrow δ1-band gives rise to a large value of N(0), but a small value of I2; while the σ-band gives rise to a large value of I2, but a small value of N(0). As a result, the product N(0)I2 does not follow the behavior of N(0) even qualitatively, and it possesses a maximum far from the peak in N(0). Following this calculation, and previous calculations for the δ2 and σ-bands, an approximate relationship is developed for the contribution λito λ, coming from the various sub-bands of the 3d band, depending on the individual width of the sub-band, and its contribution to the density of states.
UR - http://www.scopus.com/inward/record.url?scp=0020707247&partnerID=8YFLogxK
U2 - 10.1016/0379-6779(83)90035-8
DO - 10.1016/0379-6779(83)90035-8
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AN - SCOPUS:0020707247
SN - 0379-6779
VL - 5
SP - 217
EP - 228
JO - Synthetic Metals
JF - Synthetic Metals
IS - 3-4
ER -