We show that an attractive interaction between two electrons confined to the surface of a sphere gives rise to a bound state, no matter how weak the interaction is. We explore the similarity between a sphere and a (two-dimensional) plane as far as pairing properties are concerned. We also discuss the relevance of the model to a recently discovered superconductor, alkali-metal-doped C60. © 1992 The American Physical Society
URL:http://link.aps.org/doi/10.1103/PhysRevLett.77.1127 DOI:10.1103/PhysRevLett.77.1127The relative...
The discovery in 1991 of high temperature superconductivity (SC) in A3C60 compounds, where A is an a...
This paper contains a review of the physical properties of the undoped and alkali-doped C60 material...
F104-111In this paper, I discuss and summarise the electron correlation based theory of the normal a...
A perimeter model for the [pi] electrons of C60 is developed and implemented within the independent ...
The trivalent alkali fulleride solids of generic composition A3C60, where C60 is the fullerene molec...
Part I. In order to interpret and predict the unusual chemical and physical properties of the C_(60)...
Using electronic states and phonon states from the first-principles calculations and including both ...
cited By 43International audienceThe electric first hyperpolarizabilities (β) of a representative se...
Abstract The electron pairing mechanism leading to superconducting state in K3C60 fullerenes is expl...
The alkali fullerides, A3C60 (A = alkali metal) are molecular superconductors that undergo a transit...
The trivalent alkali fulleride solids of generic composition A(3)C(60), where C-60 is the fullerene ...
AbstractA discret summation method [1] has been used to calculate the van der Waals dispersion inter...
Metal doped C60 compounds comprise a class of materials, which includes insulators, conductors and s...
Alkali-doped fullerides A3C60 (A = K, Rb, Cs) are surprising materials where conventional phonon-med...
URL:http://link.aps.org/doi/10.1103/PhysRevLett.77.1127 DOI:10.1103/PhysRevLett.77.1127The relative...
The discovery in 1991 of high temperature superconductivity (SC) in A3C60 compounds, where A is an a...
This paper contains a review of the physical properties of the undoped and alkali-doped C60 material...
F104-111In this paper, I discuss and summarise the electron correlation based theory of the normal a...
A perimeter model for the [pi] electrons of C60 is developed and implemented within the independent ...
The trivalent alkali fulleride solids of generic composition A3C60, where C60 is the fullerene molec...
Part I. In order to interpret and predict the unusual chemical and physical properties of the C_(60)...
Using electronic states and phonon states from the first-principles calculations and including both ...
cited By 43International audienceThe electric first hyperpolarizabilities (β) of a representative se...
Abstract The electron pairing mechanism leading to superconducting state in K3C60 fullerenes is expl...
The alkali fullerides, A3C60 (A = alkali metal) are molecular superconductors that undergo a transit...
The trivalent alkali fulleride solids of generic composition A(3)C(60), where C-60 is the fullerene ...
AbstractA discret summation method [1] has been used to calculate the van der Waals dispersion inter...
Metal doped C60 compounds comprise a class of materials, which includes insulators, conductors and s...
Alkali-doped fullerides A3C60 (A = K, Rb, Cs) are surprising materials where conventional phonon-med...
URL:http://link.aps.org/doi/10.1103/PhysRevLett.77.1127 DOI:10.1103/PhysRevLett.77.1127The relative...
The discovery in 1991 of high temperature superconductivity (SC) in A3C60 compounds, where A is an a...
This paper contains a review of the physical properties of the undoped and alkali-doped C60 material...