Using electronic states and phonon states from the first-principles calculations and including both conventional electron-phonon charge coupling and Jahn-Teller coupling, we predict T(c) and other superconducting properties. The only adjustable parameter in the theory is the screening length, R(sc). Using R(sc) = 0.8-1.0 Å, we find excellent agreement with experiment for T(c) (16-18 K), pressure dependence of T(c) (ΔT(c) = -6 to - 10 K for 1 GPa), and 12C to 13C isotope shift (α(C) = 0.2); experimental values: 19 K, -7 K, and 0.3, respectively .link_to_subscribed_fulltex
Cs3C60 is an antiferromagnetic insulator that under pressure (P) becomes metallic and superconductin...
We present a detailed investigation of the surface electronic structure of solid K;CM, and Rb3C60 in...
K-3 picene is a superconducting molecular crystal with a critical temperature of T-c = 7 or 18 K, de...
Using electronic states and phonon states from the first-principles calculations and including both ...
Abstract The electron pairing mechanism leading to superconducting state in K3C60 fullerenes is expl...
The discovery in 1991 of high temperature superconductivity (SC) in A3C60 compounds, where A is an a...
The critical temperature (TC) of superconductivity in A3C60 compounds is generally lower smaller wit...
The critical temperature (TC) of superconductivity in A3C60 compounds is generally lower smaller wit...
A possible mechanism of superconductivity in alkali fullerides (K3C60 and Rb3C60) is proposed. Such ...
Alkali-doped fullerides A3C60 (A = K, Rb, Cs) are surprising materials where conventional phonon-med...
A superconducting mechanism for K3C60 and Ba1-xK(x)BiO3 has been suggested. This is the combining p...
The alkali fullerides, A3C60 (A = alkali metal) are molecular superconductors that undergo a transit...
In the framework of the Eliashberg formalism, we have calculated the thermodynamic properties of the...
X-ray diffraction studies show that the alkali-doped fullerene has the same structure as C60 with FC...
Cs3C60 is an antiferromagnetic insulator that under pressure (P) becomes metallic and superconductin...
Cs3C60 is an antiferromagnetic insulator that under pressure (P) becomes metallic and superconductin...
We present a detailed investigation of the surface electronic structure of solid K;CM, and Rb3C60 in...
K-3 picene is a superconducting molecular crystal with a critical temperature of T-c = 7 or 18 K, de...
Using electronic states and phonon states from the first-principles calculations and including both ...
Abstract The electron pairing mechanism leading to superconducting state in K3C60 fullerenes is expl...
The discovery in 1991 of high temperature superconductivity (SC) in A3C60 compounds, where A is an a...
The critical temperature (TC) of superconductivity in A3C60 compounds is generally lower smaller wit...
The critical temperature (TC) of superconductivity in A3C60 compounds is generally lower smaller wit...
A possible mechanism of superconductivity in alkali fullerides (K3C60 and Rb3C60) is proposed. Such ...
Alkali-doped fullerides A3C60 (A = K, Rb, Cs) are surprising materials where conventional phonon-med...
A superconducting mechanism for K3C60 and Ba1-xK(x)BiO3 has been suggested. This is the combining p...
The alkali fullerides, A3C60 (A = alkali metal) are molecular superconductors that undergo a transit...
In the framework of the Eliashberg formalism, we have calculated the thermodynamic properties of the...
X-ray diffraction studies show that the alkali-doped fullerene has the same structure as C60 with FC...
Cs3C60 is an antiferromagnetic insulator that under pressure (P) becomes metallic and superconductin...
Cs3C60 is an antiferromagnetic insulator that under pressure (P) becomes metallic and superconductin...
We present a detailed investigation of the surface electronic structure of solid K;CM, and Rb3C60 in...
K-3 picene is a superconducting molecular crystal with a critical temperature of T-c = 7 or 18 K, de...