Cs3C60 is an antiferromagnetic insulator that under pressure (P) becomes metallic and superconducting below Tc = 38 K. The superconducting dome present in the T − P phase diagram close to a magnetic state reminds what found in superconducting cuprates and pnictides, strongly suggesting that superconductivity is not of the conventional Bardeen-Cooper-Schrieffer (BCS) type We investigate the insulator to metal transition induced by pressure in Cs3C60 by means of infrared spectroscopy supplemented by Dynamical Mean-Field Theory calculations. The insulating compound is driven towards a metallic-like behaviour, while strong correlations survive in the investigated pressure range. The metallization process is accompanied by an enhancement of the ...
Metal doped C60 compounds comprise a class of materials, which includes insulators, conductors and s...
The intermediate phases Cs3+alphaC60 (alpha=0.0-1.0), have been prepared, and their structure and ph...
The work reported in this thesis systematically investigates the structural, electronic and/or magne...
Cs3C60 is an antiferromagnetic insulator that under pressure (P) becomes metallic and superconductin...
Cs$_3$C$_{60}$ is an antiferromagnetic insulator that under pressure (P) becomes metallic and superc...
The discovery in 1991 of high temperature superconductivity (SC) in A3C60 compounds, where A is an a...
Cs3C60 in the A15 structure is an antiferromagnet at ambient pressure in contrast with other super-c...
Cs3C60 is a correlated superconductor under pressure, but an insulator under ambient conditions. The...
The alkali fullerides, A3C60 (A = alkali metal) are molecular superconductors that undergo a transit...
The alkali fullerides, A3C60 (A = alkali metal) are molecular superconductors that undergo a transit...
Using electronic states and phonon states from the first-principles calculations and including both ...
This thesis outlines new research findings into the solid-state properties of selected alkali- and a...
The body-centered cubic A15-structured cesium fulleride Cs3C60 is not superconducting at ambient pre...
Alkali-doped fullerides A3C60 (A = K, Rb, Cs) are surprising materials where conventional phonon-med...
Metal doped C60 compounds comprise a class of materials, which includes insulators, conductors and s...
The intermediate phases Cs3+alphaC60 (alpha=0.0-1.0), have been prepared, and their structure and ph...
The work reported in this thesis systematically investigates the structural, electronic and/or magne...
Cs3C60 is an antiferromagnetic insulator that under pressure (P) becomes metallic and superconductin...
Cs$_3$C$_{60}$ is an antiferromagnetic insulator that under pressure (P) becomes metallic and superc...
The discovery in 1991 of high temperature superconductivity (SC) in A3C60 compounds, where A is an a...
Cs3C60 in the A15 structure is an antiferromagnet at ambient pressure in contrast with other super-c...
Cs3C60 is a correlated superconductor under pressure, but an insulator under ambient conditions. The...
The alkali fullerides, A3C60 (A = alkali metal) are molecular superconductors that undergo a transit...
The alkali fullerides, A3C60 (A = alkali metal) are molecular superconductors that undergo a transit...
Using electronic states and phonon states from the first-principles calculations and including both ...
This thesis outlines new research findings into the solid-state properties of selected alkali- and a...
The body-centered cubic A15-structured cesium fulleride Cs3C60 is not superconducting at ambient pre...
Alkali-doped fullerides A3C60 (A = K, Rb, Cs) are surprising materials where conventional phonon-med...
Metal doped C60 compounds comprise a class of materials, which includes insulators, conductors and s...
The intermediate phases Cs3+alphaC60 (alpha=0.0-1.0), have been prepared, and their structure and ph...
The work reported in this thesis systematically investigates the structural, electronic and/or magne...