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Random Walk on a Random Rough Surface: Conservation Law, Dangerous Irrelevant Operator and Non-conventional Renormalization Group. / Антонов, Николай Викторович; Какинь, Полина Игоревна; Лучин, Александр Юрьевич.

в: Journal of Statistical Physics, Том 193, № 5, 57, 08.05.2026.

Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование

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@article{c1dccf0113ba48d2a6d2aaa89f300cf9,
title = "Random Walk on a Random Rough Surface: Conservation Law, Dangerous Irrelevant Operator and Non-conventional Renormalization Group",
abstract = "The long-time, large-distance behaviour of a randomly walking particle on a random rough surface in a uniform gravitational field is studied by means of the field-theoretic renormalization group (RG). The random walk is governed by the Fokker–Planck equation for the particle{\textquoteright}s probability distribution function, while the surface is described by the conserved Kardar–Parisi–Zhang (CKPZ) model due to Sun, Guo and Grant [Phys. Rev. A 40 6763 (1989)]. The corresponding field-theoretic model is logarithmic at d=2 and is shown to be multiplicatively renormalizable. The standard RG analysis based on the minimal subtraction scheme (where the ultraviolet divergences have the form of the poles in ε=2-d) reveals no infrared (IR) attractive fixed points. However, it shows that a certain IR irrelevant (in the sense of Wilson) term (composite operator) in the corresponding De Dominicis–Janssen action functional, necessarily omitted in that scheme, is in fact inevitably needed to exhaustively describe the IR behaviour of the relevant Green{\textquoteright}s functions. Thus, we use a non-conventional formulation of the renormalization scheme in fixed d dimensions, in which that operator is included from the very beginning into the action functional and is treated on the equal footing with the other terms. That scheme reveals at least one nontrivial IR attractive fixed point, elusive in the standard RG approach. The resulting asymptotic scaling expressions appear rather cumbersome, as they simultaneously involve two different critical dimensions of time/frequency (so-called weak scaling) and describe several different asymptotic sub-domains of the whole IR asymptotic region.",
keywords = "Conservation laws, Critical dynamics, Dangerous irrelevant operator, Kinetic roughening, Random walks, Renormalization group, Weak scaling behaviour",
author = "Антонов, {Николай Викторович} and Какинь, {Полина Игоревна} and Лучин, {Александр Юрьевич}",
year = "2026",
month = may,
day = "8",
doi = "10.1007/s10955-026-03598-y",
language = "English",
volume = "193",
journal = "Journal of Statistical Physics",
issn = "0022-4715",
publisher = "Springer Nature",
number = "5",

}

RIS

TY - JOUR

T1 - Random Walk on a Random Rough Surface: Conservation Law, Dangerous Irrelevant Operator and Non-conventional Renormalization Group

AU - Антонов, Николай Викторович

AU - Какинь, Полина Игоревна

AU - Лучин, Александр Юрьевич

PY - 2026/5/8

Y1 - 2026/5/8

N2 - The long-time, large-distance behaviour of a randomly walking particle on a random rough surface in a uniform gravitational field is studied by means of the field-theoretic renormalization group (RG). The random walk is governed by the Fokker–Planck equation for the particle’s probability distribution function, while the surface is described by the conserved Kardar–Parisi–Zhang (CKPZ) model due to Sun, Guo and Grant [Phys. Rev. A 40 6763 (1989)]. The corresponding field-theoretic model is logarithmic at d=2 and is shown to be multiplicatively renormalizable. The standard RG analysis based on the minimal subtraction scheme (where the ultraviolet divergences have the form of the poles in ε=2-d) reveals no infrared (IR) attractive fixed points. However, it shows that a certain IR irrelevant (in the sense of Wilson) term (composite operator) in the corresponding De Dominicis–Janssen action functional, necessarily omitted in that scheme, is in fact inevitably needed to exhaustively describe the IR behaviour of the relevant Green’s functions. Thus, we use a non-conventional formulation of the renormalization scheme in fixed d dimensions, in which that operator is included from the very beginning into the action functional and is treated on the equal footing with the other terms. That scheme reveals at least one nontrivial IR attractive fixed point, elusive in the standard RG approach. The resulting asymptotic scaling expressions appear rather cumbersome, as they simultaneously involve two different critical dimensions of time/frequency (so-called weak scaling) and describe several different asymptotic sub-domains of the whole IR asymptotic region.

AB - The long-time, large-distance behaviour of a randomly walking particle on a random rough surface in a uniform gravitational field is studied by means of the field-theoretic renormalization group (RG). The random walk is governed by the Fokker–Planck equation for the particle’s probability distribution function, while the surface is described by the conserved Kardar–Parisi–Zhang (CKPZ) model due to Sun, Guo and Grant [Phys. Rev. A 40 6763 (1989)]. The corresponding field-theoretic model is logarithmic at d=2 and is shown to be multiplicatively renormalizable. The standard RG analysis based on the minimal subtraction scheme (where the ultraviolet divergences have the form of the poles in ε=2-d) reveals no infrared (IR) attractive fixed points. However, it shows that a certain IR irrelevant (in the sense of Wilson) term (composite operator) in the corresponding De Dominicis–Janssen action functional, necessarily omitted in that scheme, is in fact inevitably needed to exhaustively describe the IR behaviour of the relevant Green’s functions. Thus, we use a non-conventional formulation of the renormalization scheme in fixed d dimensions, in which that operator is included from the very beginning into the action functional and is treated on the equal footing with the other terms. That scheme reveals at least one nontrivial IR attractive fixed point, elusive in the standard RG approach. The resulting asymptotic scaling expressions appear rather cumbersome, as they simultaneously involve two different critical dimensions of time/frequency (so-called weak scaling) and describe several different asymptotic sub-domains of the whole IR asymptotic region.

KW - Conservation laws

KW - Critical dynamics

KW - Dangerous irrelevant operator

KW - Kinetic roughening

KW - Random walks

KW - Renormalization group

KW - Weak scaling behaviour

UR - https://www.mendeley.com/catalogue/fbb09397-ab01-3468-8685-c6a491a6b5d3/

U2 - 10.1007/s10955-026-03598-y

DO - 10.1007/s10955-026-03598-y

M3 - Article

VL - 193

JO - Journal of Statistical Physics

JF - Journal of Statistical Physics

SN - 0022-4715

IS - 5

M1 - 57

ER -

ID: 153550943