Kinetic Roughening in Turbulent Environment: Spatially Quenched Kardar–Parisi–Zhang Model and Navier–Stokes Equation

Using field-theoretic renormalization group analysis, we study the Kardar–Parisi–Zhang equation of random surface growth with a spatially quenched random noise taking into account turbulent environment described by the Navier–Stokes equation. The latter is taken in the form that allows to model both macroscopic shaking of the fluid and fully turbulent flow. After establishing multiplicative renormalizability of the constructed action functional with additional non-linearity, we perform one-loop calculations (to the leading order in $$\varepsilon = 4 - d$$ and $$y$$ where $$d$$ is the space dimension) and find three sets of renormalization group equations’ fixed points: Gaussian fixed point (regime of ordinary diffusion), a curve of fixed points (macroscopic shaking) with infrared attractive segment, and a surface of fixed points for a special case $$\varepsilon = y$$ that also involved infrared attractive area. We also investigate marginal values of the coupling constants to look for “hidden” fixed points.

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Publication Details

Journal
Physics of Particles and Nuclei
Published
2025-10-25
DOI
https://doi.org/10.1134/s1063779625700467
Primary Topic
Fluid Dynamics and Turbulent Flows
Type
article
Field-Weighted Citation Impact
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article

Kinetic Roughening in Turbulent Environment: Spatially Quenched Kardar–Parisi–Zhang Model and Navier–Stokes Equation

P. I. Kakin, M. A. Reiter, N. V. Antonov, N. M. Gulitskiy
Physics of Particles and Nuclei
Fluid Dynamics and Turbulent Flows
article

Kinetic Roughening in Turbulent Environment: Spatially Quenched Kardar–Parisi–Zhang Model and Navier–Stokes Equation

P. I. Kakin, M. A. Reiter, N. V. Antonov, N. M. Gulitskiy
article en

Abstract

Using field-theoretic renormalization group analysis, we study the Kardar–Parisi–Zhang equation of random surface growth with a spatially quenched random noise taking into account turbulent environment described by the Navier–Stokes equation. The latter is taken in the form that allows to model both macroscopic shaking of the fluid and fully turbulent flow. After establishing multiplicative renormalizability of the constructed action functional with additional non-linearity, we perform one-loop calculations (to the leading order in $$\varepsilon = 4 - d$$ and $$y$$ where $$d$$ is the space dimension) and find three sets of renormalization group equations’ fixed points: Gaussian fixed point (regime of ordinary diffusion), a curve of fixed points (macroscopic shaking) with infrared attractive segment, and a surface of fixed points for a special case $$\varepsilon = y$$ that also involved infrared attractive area. We also investigate marginal values of the coupling constants to look for “hidden” fixed points.

Physics of Particles and NucleiVol. 56(6)
St Petersburg University (RU), Joint Institute for Nuclear Research (RU)
Openalex Percentile: Top 67%
Fluid Dynamics and Turbulent Flows
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