Non-equilibrium behavior at a liquid-gas critical point

European Physical Journal B

Volumn 28, Issue 4, 2002, Pages 423-440

  Santos, J E ^a   Tauber U C ^b  

^a HAHN MEITNER INSTITUT   (Germany)

^b VIRGINIA POLYTECHNIC INSTITUTE AND STATE UNIVERSITY   (United States)

Author keywords

05.70.Ln Non equilibrium thermodynamics, irreversible processes; 64.60.Ak Renormalization group, fractal, and percolation studies of phase transitions; 64.60.Ht Dynamic critical phenomena

Indexed keywords

EID: 19044362302     PISSN: 14346028     EISSN: None     Source Type: Journal    
DOI: 10.1140/epjb/e2002-00246-2     Document Type: Article

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35. Note that in the cases usually discussed in static critical phenomena, anisotropy is introduced in the order parameter space, e.g. by adding an easy axis energy term to the Hamiltonian. It is the very absence of detailed-balance constraints that gives us this additional freedom of introducing spatial anisotropy in the noise correlations here
36. In the equilibrium theory, this is a very natural choice, as the transverse currents are non-critical modes. Thus their static response is only weakly temperature-dependent and essentially constant near the critical point
37. 0 as the inverse of equation (3.17) here. The subsequent RG analysis is of course independent of this choice
38. 0 finite
39. 0j̃j (q, ω) in the main text
40. 0
41. ψ = Z = 1 holds only to one-loop order, i.e., the susceptibility (and consequently the exponent η) acquires higher order corrections
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51. 0ψ̃[j̃▽⊥ψ](-q,-ω)]
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