2012
DOI: 10.1016/j.physleta.2012.10.009
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On non-multiaffine consistent-around-the-cube lattice equations

Abstract: We show that integrable involutive maps, due to the fact they admit three integrals in separated form, can give rise to equations, which are consistent around the cube and which are not in the multiaffine form assumed in papers [1,2]. Lattice models, which are discussed here, are related to the lattice potential KdV equation by nonlocal transformations (discrete quadratures).

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Cited by 36 publications
(71 citation statements)
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“…Entwining maps associated with the H B III Yang-Baxter map The invariants that were derived in [44,45,47,56],…”
Section: Entwining Maps Associated With the H A III Yang-baxter Map Tmentioning
confidence: 99%
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“…Entwining maps associated with the H B III Yang-Baxter map The invariants that were derived in [44,45,47,56],…”
Section: Entwining Maps Associated With the H A III Yang-baxter Map Tmentioning
confidence: 99%
“…The invariants in separated variables that appear inTable 10, were firstly introduced, in a different context, in[44,45,47,56]. Note that the invariants H1, H2 for tH A III (k) iwere also given in[50].…”
mentioning
confidence: 99%
“…The six bottom members of the list, namely (Q1 δ , A2, A1 δ , H3 δ , H2, H1) admit a Lie point symmetry group. The existence of the Lie point symmetry group allows one to reformulate these six members of the list as systems of difference equations defined on the edges of a quadrangle of the Z 2 graph [40], we refer to these systems shortly as bond systems [19,25,24,28,27]. The hallmark of integrability of the bond systems is the 3-dimensional compatibility in analogy with the consistency-around-the-cube [37] of the corresponding quad-equations.…”
Section: Introductionmentioning
confidence: 99%
“…System (28) is integrable with Lax representation L a (p 01 , q 01 , q 11 , r 11 , τ 01 , θ 11 )L b (p, q, q 01 , r 01 , τ, θ 01 ) = L b (p 10 , q 10 , q 11 , r 11 , τ 10 , θ 11 )L a (p, q, q 10 , r 10 , τ, θ 10 ), (29) where L a (p, q, q 10 , r 10 , τ, θ 10 ) :=     −q 10 1 0 0 −r 10 0 1 0 a − pq 10 − qr 10 − τ θ 10 − λ p q τ −θ 10 0 0 1…”
Section: Step III : Squeeze Down To Grassmann Extension Of the Boussimentioning
confidence: 99%