2020
DOI: 10.1007/jhep07(2020)223
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Boost generator in AdS3 integrable superstrings for general braiding

Abstract: In this paper we find a host of boost operators for a very general choice of coproducts in AdS 3-inspired scattering theories, focusing on the massless sector, with and without an added trigonometric deformation. We find that the boost coproducts are exact symmetries of the R-matrices we construct, besides fulfilling the relations of modified Poincaré-type superalgebras. In the process, we discover an ambiguity in determining the boost coproduct which allows us to derive differential constraints on our R-matri… Show more

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Cited by 6 publications
(4 citation statements)
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References 85 publications
(142 reference statements)
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“…More generally given some bialgebra A we require that ∆ op (a)R(u, v) = R(u, v)∆(a) where ∆ and ∆ op denote the coproduct and opposite coproduct related by conjugation on A, respectively. In many cases this is enough to completely fix R up to a small number of functions, drastically simplifying the construction, as was demonstrated in the case of AdS/CFT integrable systems [15][16][17][18][19][20][21][22], see also [23] for recent developments using this approach. Of course, this approach first requires one to know what the corresponding symmetry is and there are R-matrices which may have no such symmetry at all.…”
Section: Introductionmentioning
confidence: 99%
“…More generally given some bialgebra A we require that ∆ op (a)R(u, v) = R(u, v)∆(a) where ∆ and ∆ op denote the coproduct and opposite coproduct related by conjugation on A, respectively. In many cases this is enough to completely fix R up to a small number of functions, drastically simplifying the construction, as was demonstrated in the case of AdS/CFT integrable systems [15][16][17][18][19][20][21][22], see also [23] for recent developments using this approach. Of course, this approach first requires one to know what the corresponding symmetry is and there are R-matrices which may have no such symmetry at all.…”
Section: Introductionmentioning
confidence: 99%
“…More generally given some bialgebra A we require that ∆ op (a)R(u, v) = R(u, v)∆(a) where ∆ and ∆ op denote the coproduct and opposite coproduct on A, respectively, cf the general discussion in section (3). In many cases this is enough to completely fix R up to a small number of functions, drastically simplifying the construction, as was demonstrated in the case of AdS/CFT integrable systems [19,[199][200][201][202][203][204][205]. Of course, this approach first requires one to know what the corresponding symmetry is and there are R-matrices which may have no such symmetry at all.…”
Section: Local Charges and Boost Automorphismmentioning
confidence: 99%
“…We believe that it must be possible to repeat our analysis substituting the mixed-flux R-matrix, although it will probably require a good deal of work to include the general k-dependence. This is because the functions become more complicated, and we do not have (discovered yet) all the nice properties of the (mixed-flux analog of the) Zamolodchikov dressing factor [55]. We are planning to study this problem in future work.…”
Section: Future Investigationmentioning
confidence: 99%