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A hierarchy of integrable PDEs in 2+1 dimensions associated with 2 - dimensional vector fields
Exactly Solvable and Integrable Systems · Submitted 24 Nov 2006
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We introduce a hierarchy of integrable PDEs in 2+1 dimensions arising from the commutation of 2-dimensional vector fields.
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The abstract, sentence by sentence
We introduce a hierarchy of integrable PDEs in 2+1 dimensions arising from the commutation of 2-dimensional vector fields. We also solve the associated Cauchy problems, using the recently developed Inverse Scattering Transform for 1-parameter families of multidimensional vector fields.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We introduce a hierarchy of integrable PDEs in 2+1 dimensions arising from the commutation of 2-dimensional vector fields. | contribution 1.00 | 0.94 | 0.54 | asserted 1.00 |
| s1 | We also solve the associated Cauchy problems, using the recently developed Inverse Scattering Transform for 1-parameter families of multidimensional vector fields. | contribution 0.60 | 0.92 | 0.24 | asserted 1.00 |
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The paper
Original abstract
We introduce a hierarchy of integrable PDEs in 2+1 dimensions arising from the commutation of 2-dimensional vector fields. We also solve the associated Cauchy problems, using the recently developed Inverse Scattering Transform for 1-parameter families of multidimensional vector fields.
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How the literature uses it
3 arXiv papers cite this in 6 sentences
Papers citing it · 2 sentences without a confident label
Uses its method or tool 1 paper
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To obtain coverings of [ref], we consider the following scheme applied before, for example, in [ref] , cf. also [ref] : 1) The nonlocal variable $w$ given by the Lax pair [ref] is expanded in a formal series in the spectral parameter $λ$, resp. $μ$: [equation] 2) By substituting this expansion into the Lax pair [ref] and eliminating the parameter $λ$, resp. $μ$, we get an infinite series of nonlocal quantities $w_i$, $i ∈Z$. 3) To achieve the proper definition of nonlocal variables $w_i$, we consider two reductions of the series $w_i$: (a) the negative reduction $w_i=0$ for $i>0$ and (b) the positive reduction $w_i=0$ for $i<0$. 4) In this way, we arrive at the following three inequivalent infinite-dimensional coverings $τ^q$, $τ^m$ and $τ^r$ (given in the form of Lax pairs) with the nonlocal variables $q_α,m_α,r_β$ respectively, where: [equation]
On recursion operators for full-fledged nonlocal symmetries of the reduced quasi-classical self-dual Yang-Mills equation · Coverings and the recursion operator for full-fledged nonlocal symmetries of the rYME · 0.92
Compares with it 2 papers
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This is nothing but the recursion operator found in [ref] rewritten as a Bäcklund auto-transformation for ([ref]).
A Simple Construction of Recursion Operators for Multidimensional Dispersionless Integrable Systems · Example 1 · 0.99
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Note that in a number of examples, where the recursion operators are already known, e.g. the Pavlov equation [ref] , our method produces the recursion operators which are inverse to the known ones.
Recursion operators for dispersionless integrable systems in any dimension · The general approach · 0.97
Cites it as background 1 paper
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Now turn to dispersionless multidimensional systems which can be written as a commutativity condition for a pair of first-order linear scalar differential operators with no free terms (i.e., vector fields) and no derivatives with respect to the spectral parameter; see e.g. [ref] and references therein for more information on such systems.
Recursion operators for dispersionless integrable systems in any dimension · Introduction · 1.00
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