A new stable compound Ba3C60 is reported in the Ba-C60 phase diagram. Rietveld refinement of x-ray powder diffraction data shows that this compound has the A15 structure with a lattice constant of 11.34. The Pm3̄n space group implies a perfect alternating orientational order for the C60 molecules, not previously observed in doped fullerite structures. The relative stability of the A15 phase over the fully intercalated fcc structure can be explained by a simple model involving the Madelung energy differences, orientation dependence of the C60-cation interaction energy, and distortion-induced relaxational energy gains
The room-temperature face-centered cubic (FCC-a0) phase as well as the low-temperature simple cubic ...
This thesis outlines new research findings into the solid-state properties of selected alkali- and a...
Alkali-doped fullerides A3C60 (A = K, Rb, Cs) are surprising materials where conventional phonon-med...
The electronic structure of BaxC60 fullerides was studied theoretically under special consideration ...
The band structure of Ba3C60 has been modeled by a crystal orbital (CO) formalism of the intermediat...
In the present thesis, I discuss some of the current advances in research in the field of the solid ...
The solid state structures assumed by fullerenes and their derivatives have been studied. The princi...
Evidence is provided for a new low-temperature superstructure in pure C60; its structure can be desc...
We correlate the presence or absence of high-order modulated structures in solid C60 with the differ...
Much of the interest in C60 and its derivatives arises from the elegant, nearly spherical molecular ...
X-ray diffraction and differential scanning calorimetry of MxC60, with x∼1 and M=K, Rb, or Cs, revea...
The band structure of Ba5C60 has been studied by a crystal orbital (CO) approach of the intermediate...
We have grown crystals of the carbon structure C60 by sublimation. In contrast to solution-grown cry...
The structure of (CO)xC60 (x=0.67) has been determined by x-ray powder diffraction at 25 K. CO is fo...
The room-temperature face-centered cubic (FCC-a0) phase as well as the low-temperature simple cubic ...
The room-temperature face-centered cubic (FCC-a0) phase as well as the low-temperature simple cubic ...
This thesis outlines new research findings into the solid-state properties of selected alkali- and a...
Alkali-doped fullerides A3C60 (A = K, Rb, Cs) are surprising materials where conventional phonon-med...
The electronic structure of BaxC60 fullerides was studied theoretically under special consideration ...
The band structure of Ba3C60 has been modeled by a crystal orbital (CO) formalism of the intermediat...
In the present thesis, I discuss some of the current advances in research in the field of the solid ...
The solid state structures assumed by fullerenes and their derivatives have been studied. The princi...
Evidence is provided for a new low-temperature superstructure in pure C60; its structure can be desc...
We correlate the presence or absence of high-order modulated structures in solid C60 with the differ...
Much of the interest in C60 and its derivatives arises from the elegant, nearly spherical molecular ...
X-ray diffraction and differential scanning calorimetry of MxC60, with x∼1 and M=K, Rb, or Cs, revea...
The band structure of Ba5C60 has been studied by a crystal orbital (CO) approach of the intermediate...
We have grown crystals of the carbon structure C60 by sublimation. In contrast to solution-grown cry...
The structure of (CO)xC60 (x=0.67) has been determined by x-ray powder diffraction at 25 K. CO is fo...
The room-temperature face-centered cubic (FCC-a0) phase as well as the low-temperature simple cubic ...
The room-temperature face-centered cubic (FCC-a0) phase as well as the low-temperature simple cubic ...
This thesis outlines new research findings into the solid-state properties of selected alkali- and a...
Alkali-doped fullerides A3C60 (A = K, Rb, Cs) are surprising materials where conventional phonon-med...