2004
DOI: 10.1103/physrevb.69.134301
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Nonequilibrium critical relaxation in the presence of extended defects

Abstract: We study nonequilibrium critical relaxation properties of systems with quenched extended defects, correlated in ε d dimensions and randomly distributed in the remaining d − ε d dimensions. Using a field-theoretic renormalization-group approach, we find the scaling behavior of the nonequilibrium response and correlation functions and calculate the initial slip exponents θ and θ ′ , which describe the growth of correlations during the initial stage of the critical relaxation, in the two-loop approximation.

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Cited by 14 publications
(21 citation statements)
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“…The exponents describing the correlation functions in the LR QLRO phase are given by Eqs. (29) and (30). Note that below d lc we have η > 0.…”
Section: Long-range Random Anisotropy O(n ) Modelmentioning
confidence: 95%
“…The exponents describing the correlation functions in the LR QLRO phase are given by Eqs. (29) and (30). Note that below d lc we have η > 0.…”
Section: Long-range Random Anisotropy O(n ) Modelmentioning
confidence: 95%
“…The defects are d -dimensional objects ͑hyperplanes͒ extending throughout the whole system along the coordinate x ʈ and randomly distributed in the transverse directions x Ќ with the concentration taken to be well below the percolation limit. [36][37][38] The corresponding correlator of the disorder potential can be written as…”
Section: A Generalized Columnar Disordermentioning
confidence: 99%
“…Similarly as in the former subsection 4.2.1 we give in the table 5 the values of the observables that are used in the FSS analysis. Now one can extract the correlation length critical exponent ν from the FSS of maxima of four different quantities: temperature derivatives of logarithm of magnetization and of its square D M , D M 2 (12) and of magnetic cumulants D U 4 , D U 2 (10). Corresponding plots are given in fig.…”
Section: Averaging Bmentioning
confidence: 99%