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Effects of turbulent transfer on critical behavior. / Antonov, N. V.; Kapustin, A. S.; Malyshev, A. V.

в: Theoretical and Mathematical Physics, Том 169, № 1, 2011, стр. 1470-1480.

Результаты исследований: Научные публикации в периодических изданияхстатья

Harvard

Antonov, NV, Kapustin, AS & Malyshev, AV 2011, 'Effects of turbulent transfer on critical behavior.', Theoretical and Mathematical Physics, Том. 169, № 1, стр. 1470-1480. https://doi.org/10.1007/s11232-011-0123-x

APA

Antonov, N. V., Kapustin, A. S., & Malyshev, A. V. (2011). Effects of turbulent transfer on critical behavior. Theoretical and Mathematical Physics, 169(1), 1470-1480. https://doi.org/10.1007/s11232-011-0123-x

Vancouver

Antonov NV, Kapustin AS, Malyshev AV. Effects of turbulent transfer on critical behavior. Theoretical and Mathematical Physics. 2011;169(1):1470-1480. https://doi.org/10.1007/s11232-011-0123-x

Author

Antonov, N. V. ; Kapustin, A. S. ; Malyshev, A. V. / Effects of turbulent transfer on critical behavior. в: Theoretical and Mathematical Physics. 2011 ; Том 169, № 1. стр. 1470-1480.

BibTeX

@article{b61a5b4ae4204bf7bdb7dc06c65eb68d,
title = "Effects of turbulent transfer on critical behavior.",
abstract = "Using the field theory renormalization group, we study the critical behavior of two systems subjected to turbulent mixing. The first system, described by the equilibrium model A, corresponds to the relaxational dynamics of a nonconserved order parameter. The second system is the strongly nonequilibrium reaction-diffusion system, known as the Gribov process or directed percolation process. The turbulent mixing is modeled by the stochastic Navier-Stokes equation with a random stirring force with the correlator ∞ δ(t − t′)p 4−d−y, where p is the wave number, d is the space dimension, and y is an arbitrary exponent. We show that the systems exhibit various types of critical behavior depending on the relation between y and d. In addition to known regimes (original systems without mixing and a passively advected scalar field), we establish the existence of new strongly nonequilibrium universality classes and calculate the corresponding critical dimensions to the first order of the double expansion in y and ɛ = 4 −",
keywords = "renormalization group – critical behavior – turbulent transfer",
author = "Antonov, {N. V.} and Kapustin, {A. S.} and Malyshev, {A. V.}",
year = "2011",
doi = "10.1007/s11232-011-0123-x",
language = "не определен",
volume = "169",
pages = "1470--1480",
journal = "Theoretical and Mathematical Physics (Russian Federation)",
issn = "0040-5779",
publisher = "Springer Nature",
number = "1",

}

RIS

TY - JOUR

T1 - Effects of turbulent transfer on critical behavior.

AU - Antonov, N. V.

AU - Kapustin, A. S.

AU - Malyshev, A. V.

PY - 2011

Y1 - 2011

N2 - Using the field theory renormalization group, we study the critical behavior of two systems subjected to turbulent mixing. The first system, described by the equilibrium model A, corresponds to the relaxational dynamics of a nonconserved order parameter. The second system is the strongly nonequilibrium reaction-diffusion system, known as the Gribov process or directed percolation process. The turbulent mixing is modeled by the stochastic Navier-Stokes equation with a random stirring force with the correlator ∞ δ(t − t′)p 4−d−y, where p is the wave number, d is the space dimension, and y is an arbitrary exponent. We show that the systems exhibit various types of critical behavior depending on the relation between y and d. In addition to known regimes (original systems without mixing and a passively advected scalar field), we establish the existence of new strongly nonequilibrium universality classes and calculate the corresponding critical dimensions to the first order of the double expansion in y and ɛ = 4 −

AB - Using the field theory renormalization group, we study the critical behavior of two systems subjected to turbulent mixing. The first system, described by the equilibrium model A, corresponds to the relaxational dynamics of a nonconserved order parameter. The second system is the strongly nonequilibrium reaction-diffusion system, known as the Gribov process or directed percolation process. The turbulent mixing is modeled by the stochastic Navier-Stokes equation with a random stirring force with the correlator ∞ δ(t − t′)p 4−d−y, where p is the wave number, d is the space dimension, and y is an arbitrary exponent. We show that the systems exhibit various types of critical behavior depending on the relation between y and d. In addition to known regimes (original systems without mixing and a passively advected scalar field), we establish the existence of new strongly nonequilibrium universality classes and calculate the corresponding critical dimensions to the first order of the double expansion in y and ɛ = 4 −

KW - renormalization group – critical behavior – turbulent transfer

U2 - 10.1007/s11232-011-0123-x

DO - 10.1007/s11232-011-0123-x

M3 - статья

VL - 169

SP - 1470

EP - 1480

JO - Theoretical and Mathematical Physics (Russian Federation)

JF - Theoretical and Mathematical Physics (Russian Federation)

SN - 0040-5779

IS - 1

ER -

ID: 5113957