7 pages, 3 figure, 2 figures are added, the volume changes from 4 pages to 7 pagesWithin generalized random energy models, we study the effects of energy discreteness and of entropy extensivity in the low temperature phase. At zero temperature, discreteness of the energy induces replica symmetry breaking, in contrast to the continuous case where the ground state is unique. However, when the ground state energy has an extensive entropy, the distribution of overlaps P(q) instead tends towards a single delta function in the large volume limit. Considering now the whole frozen phase, we find that P(q) varies continuously with temperature, and that state-to-state fluctuations of entropy wash out the differences between the discrete and continuou...
Many physical systems are governed by long range interactions, the main example being self-gravitati...
The probability density function (PDF) of a global measure in a large class of highly correlated sys...
An expression for the moment of the partition function valid for any finite system size N and comple...
7 pages, 3 figure, 2 figures are added, the volume changes from 4 pages to 7 pagesWithin generalized...
This work is devoted to the modeling of energy fluctuation effect on the behavior of small classical...
International audienceAs part of our study of configurational entropy in non-equilibrium systems, we...
The order parameter P(q) for disordered systems with degenerate ground states is reconsidered. We p...
Abstract. Motivated by the Lee–Yang approach to phase transitions, we study the partition function o...
15 pages, 7 figuresThe definition of a nonequilibrium temperature through generalized fluctuation-di...
We study Derrida's generalized random energy model (GREM) in the presence of uniform external field....
The proper definition of thermodynamics and the thermodynamic entropy is discussed in the light of r...
International audienceAs a contribution to the residual entropy debate for glasses, we have made sim...
We study Derrida’s generalized random energy model in the presence of uniform external field. We com...
Understanding nonequilibrium systems and the consequences of irreversibility for the system's behavi...
We postulate the existence of universal crossover functions connecting the universal parts of the en...
Many physical systems are governed by long range interactions, the main example being self-gravitati...
The probability density function (PDF) of a global measure in a large class of highly correlated sys...
An expression for the moment of the partition function valid for any finite system size N and comple...
7 pages, 3 figure, 2 figures are added, the volume changes from 4 pages to 7 pagesWithin generalized...
This work is devoted to the modeling of energy fluctuation effect on the behavior of small classical...
International audienceAs part of our study of configurational entropy in non-equilibrium systems, we...
The order parameter P(q) for disordered systems with degenerate ground states is reconsidered. We p...
Abstract. Motivated by the Lee–Yang approach to phase transitions, we study the partition function o...
15 pages, 7 figuresThe definition of a nonequilibrium temperature through generalized fluctuation-di...
We study Derrida's generalized random energy model (GREM) in the presence of uniform external field....
The proper definition of thermodynamics and the thermodynamic entropy is discussed in the light of r...
International audienceAs a contribution to the residual entropy debate for glasses, we have made sim...
We study Derrida’s generalized random energy model in the presence of uniform external field. We com...
Understanding nonequilibrium systems and the consequences of irreversibility for the system's behavi...
We postulate the existence of universal crossover functions connecting the universal parts of the en...
Many physical systems are governed by long range interactions, the main example being self-gravitati...
The probability density function (PDF) of a global measure in a large class of highly correlated sys...
An expression for the moment of the partition function valid for any finite system size N and comple...