We propose a two-stage mechanism for the rotational surface disordering phase transition of a molecular crystal, as realized in C60 fullerite. Our study, based on Monte Carlo simulations, uncovers the existence of a new intermediate regime, between a low-temperature ordered (2×2) state, and a high-temperature (1×1) disordered phase. In the intermediate regime there is partial disorder, strongest for a subset of particularly frustrated surface molecules. These concepts and calculations provide a coherent understanding of experimental observations, with possible extension to other molecular crystal surfaces
International audienceOur understanding of the atomic structure of materials relies on our ability t...
The temperature dependences of the triplet exciton, of the vibrational modes, and of the low-energy ...
We study the structure and phase behavior of fullerene-cubane C(60) x C(8)H(8) by Monte Carlo simula...
A two-stage mechanism was proposed for the rotational surface disordering phase transition of a mole...
We propose a two-stage mechanism for the rotational surface disordering phase transition of a molecu...
C60 is a model system to study molecule–surface interactions and phase transitions due to its high s...
C60 is a model system to study molecule–surface interactions and phase transitions due to its high s...
The co-crystal of C60·2CBrClH2 possesses a monoclinic (C2/m) structure at room temperature with both...
Recently, heteromolecular crystals of fullerene C60 and cubane (C8H8) have been synthesized. For som...
The co-crystal of C60·2CBrClH2 possesses a monoclinic (C2/m) structure at room temperature with both...
We present a full characterization of the orientationally disordered cocrystal of C-60 with (1,1,2)-...
The solid state structures assumed by fullerenes and their derivatives have been studied. The princi...
The surface of a crystal made of roughly spherical molecules exposes, above its bulk rotational phas...
Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)Coordenação de Aperfeiçoamento de Pesso...
International audienceOur understanding of the atomic structure of materials relies on our ability t...
International audienceOur understanding of the atomic structure of materials relies on our ability t...
The temperature dependences of the triplet exciton, of the vibrational modes, and of the low-energy ...
We study the structure and phase behavior of fullerene-cubane C(60) x C(8)H(8) by Monte Carlo simula...
A two-stage mechanism was proposed for the rotational surface disordering phase transition of a mole...
We propose a two-stage mechanism for the rotational surface disordering phase transition of a molecu...
C60 is a model system to study molecule–surface interactions and phase transitions due to its high s...
C60 is a model system to study molecule–surface interactions and phase transitions due to its high s...
The co-crystal of C60·2CBrClH2 possesses a monoclinic (C2/m) structure at room temperature with both...
Recently, heteromolecular crystals of fullerene C60 and cubane (C8H8) have been synthesized. For som...
The co-crystal of C60·2CBrClH2 possesses a monoclinic (C2/m) structure at room temperature with both...
We present a full characterization of the orientationally disordered cocrystal of C-60 with (1,1,2)-...
The solid state structures assumed by fullerenes and their derivatives have been studied. The princi...
The surface of a crystal made of roughly spherical molecules exposes, above its bulk rotational phas...
Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)Coordenação de Aperfeiçoamento de Pesso...
International audienceOur understanding of the atomic structure of materials relies on our ability t...
International audienceOur understanding of the atomic structure of materials relies on our ability t...
The temperature dependences of the triplet exciton, of the vibrational modes, and of the low-energy ...
We study the structure and phase behavior of fullerene-cubane C(60) x C(8)H(8) by Monte Carlo simula...