The entropy per particle in most Monte-Carlo simulations is size dependent due to correlated energy fluctuations. Guided by nanothermodynamics, we find a constraint for the Ising model that enhances the fluctuations and lowers the free energy, while making the entropy homogeneous, additive, and extensive. Although the average interaction energy becomes size dependent, the resulting distribution of energies provides a mechanism for the heterogeneity found in the dynamics of many materials
We investigate simultaneous effects of finite system size and global charge conservation on thermal ...
This letter concerns the extension to non-reversible systems of a relation between the statistics of...
Entropy and the fluctuation-dissipation theorem are at the heart of statistical mechan-ics near equi...
The Boltzmann factor comes from the linear change in entropy of an infinite heat bath during a loca...
Nanothermodynamics extends standard thermodynamics to facilitate finite-size effects on the scale of...
abstract: Computer simulations of the Ising model exhibit white noise if thermal fluctuations are go...
We derive a general lower bound on distributions of entropy production in interacting active matter ...
Fluctuation theorems, developed over the past 15 years, have resulted in fundamental breakthroughs i...
<p>Entropy per particle for the Ising model on a square lattice as a function of the temperature . ...
Certain fluctuations in particle number, (n), at fixed total energy, (E), lead exactly to a cut-powe...
Entropy and the fluctuation-dissipation theorem are at the heart of statistical mechan-ics near equi...
The total entropy production generated by the dynamics of an externally driven systems exchanging en...
We present a new numerical Monte Carlo approach to determine the scaling behavior of lattice field t...
The relationships among reversible Carnot cycles, the absence of perpetual motion machines, and the ...
We study theoretical issues related to the use of finite size systems in Monte Carlo simulations of ...
We investigate simultaneous effects of finite system size and global charge conservation on thermal ...
This letter concerns the extension to non-reversible systems of a relation between the statistics of...
Entropy and the fluctuation-dissipation theorem are at the heart of statistical mechan-ics near equi...
The Boltzmann factor comes from the linear change in entropy of an infinite heat bath during a loca...
Nanothermodynamics extends standard thermodynamics to facilitate finite-size effects on the scale of...
abstract: Computer simulations of the Ising model exhibit white noise if thermal fluctuations are go...
We derive a general lower bound on distributions of entropy production in interacting active matter ...
Fluctuation theorems, developed over the past 15 years, have resulted in fundamental breakthroughs i...
<p>Entropy per particle for the Ising model on a square lattice as a function of the temperature . ...
Certain fluctuations in particle number, (n), at fixed total energy, (E), lead exactly to a cut-powe...
Entropy and the fluctuation-dissipation theorem are at the heart of statistical mechan-ics near equi...
The total entropy production generated by the dynamics of an externally driven systems exchanging en...
We present a new numerical Monte Carlo approach to determine the scaling behavior of lattice field t...
The relationships among reversible Carnot cycles, the absence of perpetual motion machines, and the ...
We study theoretical issues related to the use of finite size systems in Monte Carlo simulations of ...
We investigate simultaneous effects of finite system size and global charge conservation on thermal ...
This letter concerns the extension to non-reversible systems of a relation between the statistics of...
Entropy and the fluctuation-dissipation theorem are at the heart of statistical mechan-ics near equi...