2019
DOI: 10.1007/jhep03(2019)143
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On rigidity of 3d asymptotic symmetry algebras

Abstract: We study rigidity and stability of infinite dimensional algebras which are not subject to the Hochschild-Serre factorization theorem. In particular, we consider algebras appearing as asymptotic symmetries of three dimensional spacetimes, the bms 3 , u(1) Kac-Moody and Virasoro algebras. We construct and classify the family of algebras which appear as deformations of bms 3 , u(1) Kac-Moody and their central extensions by direct computations and also by cohomological analysis. The Virasoro algebra appears as a s… Show more

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Cited by 20 publications
(12 citation statements)
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References 94 publications
(200 reference statements)
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“…For D = 3, the algebra (IV.5) for s = 0 agrees with the one found in [52,69] while for s = 1 it is the BMS 3 algebra [98,99]. For generic s it is the W (0, −s) algebra [100,101], where the supertranslations are generators with conformal weight h = s + 1.…”
Section: Bms-like Symmetriessupporting
confidence: 65%
See 1 more Smart Citation
“…For D = 3, the algebra (IV.5) for s = 0 agrees with the one found in [52,69] while for s = 1 it is the BMS 3 algebra [98,99]. For generic s it is the W (0, −s) algebra [100,101], where the supertranslations are generators with conformal weight h = s + 1.…”
Section: Bms-like Symmetriessupporting
confidence: 65%
“…For s = 1 the algebra (A.2) coincides with the standard (non-centrally extended) BMS 3 algebra [98,99], while for s = 0 the algebra (A.2) reduces to the one in [52]. For generic s, the algebra (A.2) is W (0, −s) [100,101] which may be obtained as algebraic deformation of BMS 3 [101].…”
Section: Comments and Further Developmentsmentioning
confidence: 99%
“…In the terminology used in [47], it is W (0, 0) algebra. This algebra was found as near horizon symmetry algebra of 3d black holes [17] (see also [28]).…”
Section: Jhep10(2020)107mentioning
confidence: 99%
“…66) and(3.67), define the group operation of the Maxwell-BMS 3 group through eq.(4.7). The Lie algebra maxwell-bms 3 = vect S 1 i ad vect S 1 (ab) ext (4.29) JHEP10(2019)039 defines a Maxwell extensions of the bms 3 algebra, whose bracket is defined by eq.…”
mentioning
confidence: 99%
“…For a detailed analysis of the rigidity and stability of the bms algebra in three and four dimensions based on their semi-direct sum structure, see[66,67].…”
mentioning
confidence: 99%