Evidence is provided for a new low-temperature superstructure in pure C60; its structure can be described as face-centered cubic with a lattice parameter 2a0. The superstructure is most probably the result of rotations alternatingly over +φ1 and –φ2 about one of the <111> axes of neighboring molecules along the cube directions. The experimental evidence is based on low-temperature electron diffraction.
X-ray powder diffraction studies on pure C70 and C60 solids in the temperature range 298-773 K is re...
The structure of (CO)xC60 (x=0.67) has been determined by x-ray powder diffraction at 25 K. CO is fo...
The structure of the low-temperature phase of hexagonal close-packed (hcp) grown C70 is determined f...
Evidence is provided for a new low-temperature superstructure in pure C60; its structure can be desc...
Evidence is provided for a new low-temperature superstructure in pure C60; its structure can be desc...
The phase transition in C60 and (related) lattice defects are studied by low-temperature electron mi...
The room-temperature face-centered cubic (FCC-a0) phase as well as the low-temperature simple cubic ...
The phase transition in C60 and (related) lattice defects are studied by low-temperature electron mi...
The crystal structure and defect structures of C60 material have been studied by means of X-ray diff...
The room-temperature face-centered cubic (FCC-a0) phase as well as the low-temperature simple cubic ...
We correlate the presence or absence of high-order modulated structures in solid C60 with the differ...
We have grown crystals of the carbon structure C60 by sublimation. In contrast to solution-grown cry...
Electron-spin-echo experiments at 95 GHz and 1.2 K reveal that the triplet excitation of a single cr...
We study the structure and phase behavior of fullerene-cubane C(60) x C(8)H(8) by Monte Carlo simula...
X-ray diffraction has employed to study the low temperature structural behavior of C$_{60}$ crystals...
X-ray powder diffraction studies on pure C70 and C60 solids in the temperature range 298-773 K is re...
The structure of (CO)xC60 (x=0.67) has been determined by x-ray powder diffraction at 25 K. CO is fo...
The structure of the low-temperature phase of hexagonal close-packed (hcp) grown C70 is determined f...
Evidence is provided for a new low-temperature superstructure in pure C60; its structure can be desc...
Evidence is provided for a new low-temperature superstructure in pure C60; its structure can be desc...
The phase transition in C60 and (related) lattice defects are studied by low-temperature electron mi...
The room-temperature face-centered cubic (FCC-a0) phase as well as the low-temperature simple cubic ...
The phase transition in C60 and (related) lattice defects are studied by low-temperature electron mi...
The crystal structure and defect structures of C60 material have been studied by means of X-ray diff...
The room-temperature face-centered cubic (FCC-a0) phase as well as the low-temperature simple cubic ...
We correlate the presence or absence of high-order modulated structures in solid C60 with the differ...
We have grown crystals of the carbon structure C60 by sublimation. In contrast to solution-grown cry...
Electron-spin-echo experiments at 95 GHz and 1.2 K reveal that the triplet excitation of a single cr...
We study the structure and phase behavior of fullerene-cubane C(60) x C(8)H(8) by Monte Carlo simula...
X-ray diffraction has employed to study the low temperature structural behavior of C$_{60}$ crystals...
X-ray powder diffraction studies on pure C70 and C60 solids in the temperature range 298-773 K is re...
The structure of (CO)xC60 (x=0.67) has been determined by x-ray powder diffraction at 25 K. CO is fo...
The structure of the low-temperature phase of hexagonal close-packed (hcp) grown C70 is determined f...