Detailed Information on Publication Record
2024
Extended symmetry analysis of (1+2)-dimensional fine Kolmogorov backward equation
KOVAL, Serhii D and Roman POPOVYCHBasic 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
References:
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.