2010
DOI: 10.48550/arxiv.1007.0435
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How higher-spin gravity surpasses the spin two barrier: no-go theorems versus yes-go examples

Xavier Bekaert,
Nicolas Boulanger,
Per Sundell
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Cited by 92 publications
(198 citation statements)
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“…Here the vectors |Λ s , |Λ 1 s are the vectors of zero-level and first-level gauge parameters of the abelian gauge transformations (5), which reflect the fact that the theory is the first-stage reducible gauge theory. The quantity Q in (3) is the BRST operator, constructed on the base of the constraints l 0 , l 1 , l + 1 , l 11 , l + 11 = 1 2 a +ν a + ν and contains the anticommuting ghost operators η 0 , η + 1 , η 1 , η + 11 , η 11 , P 0 , P 1 , P + 1 , P 11 , P + 11 ,…”
Section: Brst Lagrangian Formulation For Free Higher Spin Fieldsmentioning
confidence: 99%
See 1 more Smart Citation
“…Here the vectors |Λ s , |Λ 1 s are the vectors of zero-level and first-level gauge parameters of the abelian gauge transformations (5), which reflect the fact that the theory is the first-stage reducible gauge theory. The quantity Q in (3) is the BRST operator, constructed on the base of the constraints l 0 , l 1 , l + 1 , l 11 , l + 11 = 1 2 a +ν a + ν and contains the anticommuting ghost operators η 0 , η + 1 , η 1 , η + 11 , η 11 , P 0 , P 1 , P + 1 , P 11 , P + 11 ,…”
Section: Brst Lagrangian Formulation For Free Higher Spin Fieldsmentioning
confidence: 99%
“…Study of the various aspects of the higher spin fields theory is one of the topical trends in modern high-energy theoretical and mathematical physics (for a review, see, e.g. [1], [2], [4], [5], [6], [7] and the references therein). The current progress in higher spin field theory is closely related to a description of interactions between these fields.…”
Section: Introductionmentioning
confidence: 99%
“…In three space-time dimensions the situation is very different: on the one hand, Fronsdal's gauge fields with "spin" s > 1 do not propagate any local degree of freedom. 2 On the other hand, in D = 3 the Weyl tensor vanishes for any gravitational background and this suggests a possible way to avoid the no-go results for minimal coupling. This expectation was indeed confirmed by Aragone and Deser in [7].…”
Section: Introductionmentioning
confidence: 99%
“…12 In [29] a somewhat similar model was constructed by taking the associative limit of a gauge theory defined on non-associative fuzzy spaces, the difference being that in [29] the star product which does not satisfy the hermicity property (A.4) appeared instead of the Moyal product. 13 For a review of NC field theory see [30].…”
Section: Mhs Yang-mills Modelmentioning
confidence: 99%
“…[6,7,8,9]. 5 See [10,9,11,12] and reviews [13,5]. 6 One can avoid traditional no-go theorems by taking AdS spacetime as a background, allowing for Vasiliev higher spin program [15,2] to be developed, but so far only with partial success as no off-shell formulation of a consistent interacting HS QFT in d ≥ 4 exists.…”
Section: Introductionmentioning
confidence: 99%