Higher jet prolongation Lie algebras and Backlund transformations for (1+1)-dimensional PDEs
Sergey Igonin

TL;DR
This paper introduces a hierarchy of Lie algebras associated with (1+1)-dimensional PDEs, which classify all Lax pairs and zero-curvature representations, aiding in understanding Backlund transformations and PDE integrability.
Contribution
It defines a sequence of Lie algebras $F^p$ for arbitrary jet order, generalizing Wahlquist-Estabrook algebras, and applies them to classify PDEs via Backlund transformations.
Findings
Computed $F^p(E,a)$ for KdV-type equations.
Found infinite-dimensional and semisimple Lie algebras within $F^p(E,a)$.
Established a necessary condition for PDEs to be connected by Backlund transformations.
Abstract
For any (1+1)-dimensional (multicomponent) evolution PDE, we define a sequence of Lie algebras , , which are responsible for all Lax pairs and zero-curvature representations (ZCRs) of this PDE. In our construction, jets of arbitrary order are allowed. In the case of lower order jets, the algebras generalize Wahlquist-Estabrook prolongation algebras. To achieve this, we find a normal form for (nonlinear) ZCRs with respect to the action of the group of gauge transformations. One shows that any ZCR is locally gauge equivalent to the ZCR arising from a vector field representation of the algebra , where is the order of jets involved in the -part of the ZCR. More precisely, we define a Lie algebra for each nonnegative integer and each point of the infinite prolongation of the evolution PDE. So the full notation for the algebra is…
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Taxonomy
TopicsNonlinear Waves and Solitons · Advanced Topics in Algebra · Algebraic structures and combinatorial models
