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On the characteristic form of $\mathfrak{g}$-valued zero-curvature representations

Jirina Jahnova

TL;DR

This work extends the scalar conservation-law paradigm to $\mathfrak{g}$-valued zero-curvature representations (ZCRs) of PDEs in two independent variables by developing a jet-space framework and introducing the characteristic form of ZCRs. It proves that every $\mathfrak{g}$-valued ZCR admits a characteristic representative whose Maurer–Cartan condition is written in terms of an $N$-tuple of $\mathfrak{g}$-valued functions, with the restriction of this tuple on the equation manifold yielding the characteristic element; this form is preserved under gauge transformations, making it a robust normal form for ZCR classification and computation. The authors derive a new necessary condition, independent of the Maurer–Cartan equation, that characteristic representatives must satisfy in the nonabelian setting, while the abelian case reduces to the classical conservation-law picture. They also discuss computational implications, suggesting that the characteristic form can enhance searches and enable more systematic classification of ZCRs, with the KdV example illustrating non-uniqueness of representatives but equivalence of their characteristics. Overall, the paper provides a structural bridge between conservation laws and ZCRs, offering tools for both theoretical analysis and practical computation in integrable systems.

Abstract

We study $\mathfrak{g}$-valued zero-curvature representations (ZCRs) for partial differential equations in two independent variables from the perspective of their extension to the entire infinite jet space, focusing on their characteristic elements. Since conservation laws -- more precisely, conserved currents -- and their generating functions for a given equation are precisely the $\mathbb{R}$-valued ZCRs and their characteristic elements, a natural question arises: to what extent can results known for conservation laws be extended to general $\mathfrak{g}$-valued ZCRs. For a fixed matrix Lie algebra $\mathfrak{g} \subset \mathfrak{gl}(n)$, we formulate ZCRs as equivalence classes of $\mathfrak{g}$-valued function pairs on the infinite jet space that satisfy the Maurer--Cartan condition. Our main result establishes that every such ZCR admits a characteristic representative -- i.e., a representative in which the Maurer--Cartan condition takes a characteristic form -- generalizing the characteristic form known for conservation laws. This form is preserved under gauge transformations and can thus be regarded as a kind of normal form for ZCRs. We derive a new necessary condition, independent of the Maurer--Cartan equation, that must be satisfied by any characteristic representative. This condition is trivial in the abelian case but nontrivial whenever $\mathfrak{g}$ is nonabelian. These findings not only confirm structural assumptions used in previous works but also suggest potential applications in the classification and computation of ZCRs.

On the characteristic form of $\mathfrak{g}$-valued zero-curvature representations

TL;DR

This work extends the scalar conservation-law paradigm to -valued zero-curvature representations (ZCRs) of PDEs in two independent variables by developing a jet-space framework and introducing the characteristic form of ZCRs. It proves that every -valued ZCR admits a characteristic representative whose Maurer–Cartan condition is written in terms of an -tuple of -valued functions, with the restriction of this tuple on the equation manifold yielding the characteristic element; this form is preserved under gauge transformations, making it a robust normal form for ZCR classification and computation. The authors derive a new necessary condition, independent of the Maurer–Cartan equation, that characteristic representatives must satisfy in the nonabelian setting, while the abelian case reduces to the classical conservation-law picture. They also discuss computational implications, suggesting that the characteristic form can enhance searches and enable more systematic classification of ZCRs, with the KdV example illustrating non-uniqueness of representatives but equivalence of their characteristics. Overall, the paper provides a structural bridge between conservation laws and ZCRs, offering tools for both theoretical analysis and practical computation in integrable systems.

Abstract

We study -valued zero-curvature representations (ZCRs) for partial differential equations in two independent variables from the perspective of their extension to the entire infinite jet space, focusing on their characteristic elements. Since conservation laws -- more precisely, conserved currents -- and their generating functions for a given equation are precisely the -valued ZCRs and their characteristic elements, a natural question arises: to what extent can results known for conservation laws be extended to general -valued ZCRs. For a fixed matrix Lie algebra , we formulate ZCRs as equivalence classes of -valued function pairs on the infinite jet space that satisfy the Maurer--Cartan condition. Our main result establishes that every such ZCR admits a characteristic representative -- i.e., a representative in which the Maurer--Cartan condition takes a characteristic form -- generalizing the characteristic form known for conservation laws. This form is preserved under gauge transformations and can thus be regarded as a kind of normal form for ZCRs. We derive a new necessary condition, independent of the Maurer--Cartan equation, that must be satisfied by any characteristic representative. This condition is trivial in the abelian case but nontrivial whenever is nonabelian. These findings not only confirm structural assumptions used in previous works but also suggest potential applications in the classification and computation of ZCRs.

Paper Structure

This paper contains 7 sections, 12 theorems, 147 equations.

Key Result

Lemma 1

Let $\mathfrak{g}\subset\mathfrak{gl}$(n) be an arbitrary matrix Lie algebra. Then the following identity holds:

Theorems & Definitions (35)

  • Lemma 1
  • proof
  • Lemma 2
  • proof
  • Lemma 3
  • proof
  • Remark 1
  • Remark 2
  • Remark 3
  • Lemma 4
  • ...and 25 more