2005
DOI: 10.1103/physrevlett.95.100601
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Nonperturbative Fixed Point in a Nonequilibrium Phase Transition

Abstract: We apply the nonperturbative renormalization group method to a class of out-of-equilibrium phase transitions (usually called "parity-conserving" or, more properly, "generalized voter" class) which is out of the reach of perturbative approaches. We show the existence of a genuinely nonperturbative fixed point, i.e., a critical point that does not seem to be Gaussian in any dimension.

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Cited by 83 publications
(128 citation statements)
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“…When d decreases, σ P C approaches zero until F P C crosses F A in d = 4/3, where they exchange stability. Below d = 4/3, F A is hence stable, describing the absorbing phase and F P C acquires an unstable direction, thus driving a phase transition [3]. The corresponding flow diagram is depicted for d = 1 in figure 6.…”
Section: Even-barw: Universality Classmentioning
confidence: 99%
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“…When d decreases, σ P C approaches zero until F P C crosses F A in d = 4/3, where they exchange stability. Below d = 4/3, F A is hence stable, describing the absorbing phase and F P C acquires an unstable direction, thus driving a phase transition [3]. The corresponding flow diagram is depicted for d = 1 in figure 6.…”
Section: Even-barw: Universality Classmentioning
confidence: 99%
“…, the flow equations for the coupling constants λ k and σ k exhibit, in addition to the Gaussian fixed point F G = {σ = 0, λ = 0} and to the pure annihilation fixed point F A = {σ = 0, λ A = 0}, a non-perturbative solution F P C = {σ P C = 0, λ P C = 0} [3]. The latter governs an absorbing transition in dimension d < 4/3.…”
Section: Even-barw: Universality Classmentioning
confidence: 99%
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