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Discrete Lagrangian Multiforms for ABS Equations II: Tetrahedron and Octahedron Equations

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arxiv 2403.16845 v4 pith:UJYD7FYM submitted 2024-03-25 nlin.SI math-phmath.MP

classification nlin.SImath-phmath.MP
keywords equationslagrangianquadoctahedronequivalentformssystemtetrahedron
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We present four types of discrete Lagrangian 2-form associated to the integrable quad equations of the ABS list. These include the triangle Lagrangian that has traditionally been used in the Lagrangian multiform description of ABS equations, the trident Lagrangian that was central to Part I of this paper, and two Lagrangians that have not been studied in the multiform setting. Two of the Lagrangian 2-forms have the quad equations, or a system equivalent to the quad equations, as their Euler-Lagrange equations, and one produces the tetrahedron equations. This is in contrast to the triangle Lagrangian 2-form, which produces equations that are weaker than the quad equations (they are equivalent to two octahedron equations). We use relations between the Lagrangian 2-forms to prove that the system of quad equations is equivalent to the combined system of tetrahedron and octahedron equations. Furthermore, for each of the Lagrangian 2-forms, we study the double zero property of the exterior derivative. In particular, this gives a possible variational interpretation to the octahedron equations.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Discrete Lagrangian Multiforms for ABS Equations I: Quad Equations

    nlin.SI 2025-01 conditional novelty 7.0 of 10

    Trident Lagrangian 2-forms with integer-valued branch-tracking fields have corner equations equivalent to the ABS quad equations and restore almost-closure.

  2. On the geometry of Lagrangian one-forms

    math-ph 2024-12 conditional novelty 6.0 of 10

    A phase-space Lagrangian one-form with a one-step variational principle recovers the multi-time Euler-Lagrange equations and closure, and its Lie-group version makes Hamiltonian group actions variational.

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