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note
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Except for the massless q=0 mode, which is not important.
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54
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note
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2.
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55
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33645074952
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note
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In that case D >
-
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56
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33645063739
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note
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k,l(iω) and only n ≥ 2 vertices].
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57
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33645048740
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33645068209
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note
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2 to η to two loops.
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60
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33645071957
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note
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rt at the boundary. This is relevant also for the disorder case, since averaging over disorder one gets, an m=2 term with C a first derivative, B=C′/2 and A=0. This indeed is the condition for invariance of the m-1 term under the continuous global λ symmetry.
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61
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33645064299
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note
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r,-t. This is a symmetry of the unaveraged dynamical effective action. It is useful, e.g., to study [50] consequences of the accidental FDT property of the one-dimensional KPZ equation. It seems however a priori less useful in order to study the effective action once one integrates over modes, i.e., in the context of Wilson FRG (also further complications arise after averaging over disorder). It may be worth studying within the exact RG context, which is beyond the scope of the present paper.
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62
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33645094677
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note
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-1].
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63
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33645058191
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note
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g+ygeg but the contour remains to be worked out.
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64
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33645065131
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note
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-k/q. At least this is necessary condition for such droplet arguments to make sense.
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65
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18144376938
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33645083743
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note
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Note, however, that if the initial condition starts in an interval two adjacent minima and maxima which does not contains a zero of F(u), it instead converges in finite time to one of the endpoint of the interval at which η(u) vanishes. The solution in Eq. (G4) analytically continues the relaxation of the force to zero.
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70
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33645074166
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E. Frey, U. Tauber, and T. Hwa, cond-mat/9601049
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E. Frey, U. Tauber, and T. Hwa, cond-mat/9601049.
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