J 2024

Extended symmetry analysis of (1+2)-dimensional fine Kolmogorov backward equation

KOVAL, Serhii D and Roman POPOVYCH

Basic information

Original name

Extended symmetry analysis of (1+2)-dimensional fine Kolmogorov backward equation

Authors

KOVAL, Serhii D and Roman POPOVYCH

Edition

Studies in Applied Mathematics, Hoboken (USA), John Wiley and Sons, Inc. 2024, 0022-2526

Other information

Language

English

Type of outcome

Článek v odborném periodiku

Field of Study

10101 Pure mathematics

Country of publisher

United States of America

Confidentiality degree

není předmětem státního či obchodního tajemství

Impact factor

Impact factor: 2.700 in 2022

Organization unit

Mathematical Institute in Opava

UT WoS

001202807700001

Keywords in English

(1+2)-dimensional ultraparabolic linear Kolmogorov backward equations; classification of subalgebras; exact solutions; generalized symmetry; Lie reductions; point-symmetry group

Tags

Tags

International impact, Reviewed
Změněno: 29/1/2025 14:25, Mgr. Aleš Ryšavý

Abstract

V originále

Within the class of (1+2)-dimensional ultraparabolic linear equations, we distinguish a fine Kolmogorov backward equation with a quadratic diffusivity. Modulo the point equivalence, it is a unique equation within the class whose essential Lie invariance algebra is five-dimensional and nonsolvable. Using the direct method, we compute the point symmetry pseudogroup of this equation and analyze its structure. In particular, we single out its essential subgroup and classify its discrete elements. We exhaustively classify all subalgebras of the corresponding essential Lie invariance algebra up to inner automorphisms and up to the action of the essential point-symmetry group. This allowed us to classify Lie reductions and Lie invariant solutions of the equation under consideration. We also discuss the generation of its solutions using point and linear generalized symmetries and carry out its peculiar generalized reductions. As a result, we construct wide families of its solutions parameterized by an arbitrary finite number of arbitrary solutions of the (1+1)-dimensional linear heat equation or one or two arbitrary solutions of (1+1)-dimensional linear heat equations with inverse square potentials.