Nonsymmetric first-order transitions: Finite-size scaling and tests for infinite-range models

1990 ◽  
Vol 60 (5-6) ◽  
pp. 551-560 ◽  
Author(s):  
V. Privman ◽  
J. Rudnick
2014 ◽  
Vol 57 ◽  
pp. 68-72 ◽  
Author(s):  
Marco Mueller ◽  
Wolfhard Janke ◽  
Desmond A. Johnston

1992 ◽  
Vol 03 (05) ◽  
pp. 897-912 ◽  
Author(s):  
CHRISTIAN BORGS

In this paper, I give an overview over a recently developed rigorous theory of finite-size scaling near first order transitions. Leaving out details of the mathematical proofs, the main emphasis is put on the underlying physical ideas and the discussion of the validity of the results for regions which are, in the sense of mathematical rigour, not covered by the original papers. I present both the finite-size scaling for cubic systems and for long cylinders, discussing also a recent controversy which stems from our work on the finite-size scaling of the mass gap in long cylinders.


2015 ◽  
Vol 91 (5) ◽  
Author(s):  
Massimo Campostrini ◽  
Jacopo Nespolo ◽  
Andrea Pelissetto ◽  
Ettore Vicari

1995 ◽  
Vol 80 (5-6) ◽  
pp. 1433-1442 ◽  
Author(s):  
P. M. C. de Oliveira ◽  
S. M. Moss de Oliveira ◽  
C. E. Cordeiro ◽  
D. Stauffer

1993 ◽  
Vol 07 (26) ◽  
pp. 4371-4387 ◽  
Author(s):  
R. HILFER

A refined classification theory for phase transitions in thermodynamics and statistical mechanics in terms of their orders is introduced and analyzed. The refined thermodynamic classification is based on two independent generalizations of Ehrenfests traditional classification scheme. The statistical mechanical classification theory is based on generalized limit theorems for sums of random variables from probability theory and the newly defined block ensemble limit. The block ensemble limit combines thermodynamic and scaling limits and is similar to the finite size scaling limit. The statistical classification scheme allows for the first time a derivation of finite size scaling without renormalization group methods. The classification distinguishes two fundamentally different types of phase transitions. Phase transitions of order λ>1 correspond to well known equilibrium phase transitions, while phase transitions with order λ<1 represent a new class of transitions termed anequilibrium transitions. The generalized order λ varies inversely with the strength of fluctuations. First order and second order transitions play a special role in both classification schemes. First order transitions represent a limiting case separating equilibrium and anequilibrium transitions. The special role or second order transitions is shown to be related to the breakdown of hyperscaling. For anequilibrium transitions the nature of the heat bath in the canonical ensemble becomes important.


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