Microcanonical Thermodynamics: Phase Transitions in 'Small' Systems
By D. Gross. 2001
372 citations recorded by the source corpus.
Subfields: Economics and Econometrics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/a780ff6e650bfb7f2473f79046637085d5454881
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Economics and Econometrics
- Jeremy Butterfield
- Shamik Gupta
- Constantino Tsallis
- Felix Ritort
- Freddy Bouchet
- M. Rivet
- Bernard Borderie
- Arak M. Mathai
In Statistical and Nonlinear Physics
- Jeremy Butterfield
- Shamik Gupta
- Constantino Tsallis
- Felix Ritort
- Freddy Bouchet
- M. Rivet
- D. Mukamel
- Bernard Borderie
Citations in the corpus
- Thermodynamics and dynamics of systems with long-range interactions (2010, background): “, clusters of atoms) has been discussed in a number of studies [34], [35], [36], [37].”
- Less is Different: Emergence and Reduction Reconciled (2011, background): “But by way of emphasizing how open all these issues are, I note that some physicists have developed frameworks for understanding phase transitions without taking the thermodynamic limit (Gross (2001)).”
- What should a statistical mechanics satisfy to reflect nature (2004, background): “For the microcanonical ensemble, the situation can in fact be more complex (see, for instance [5]).”
- Nonequilibrium fluctuations in small systems: From physics to biology (2007, background): “ystems are collections of many molecules we expect that the same laws that have been found to be applicable in macroscopic systems are also valid in small systems containing a few number of molecules [1, 2]. Yet, the phenomena that we will observe in the two regimes will be different. Fluctuations in”
- Nuclear multifragmentation and phase transition for hot nuclei (2008, background): “The energetic cost paid to produce surfaces is a decrease of the microcanonical temperature when the excitation energy increases and consequently the appearance of a negative microcanonical heat capacity [200, 202] as a specific signature of a first order phase transition for finite systems.”