1979
DOI: 10.1016/0370-2693(79)90808-6
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Consistency problems of hypergravity

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Cited by 278 publications
(390 citation statements)
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“…Therefore, the construction of the consistent lagrangian theory of conformal higher spin fields (achieved in this paper) is an important step towards solution of the higher spin interaction problem [5] (see Sec. (2.2) below for a little bit more detailed reference to the higher spin problem).…”
Section: Conclusion 119 1 Introduction and Statement Of The Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Therefore, the construction of the consistent lagrangian theory of conformal higher spin fields (achieved in this paper) is an important step towards solution of the higher spin interaction problem [5] (see Sec. (2.2) below for a little bit more detailed reference to the higher spin problem).…”
Section: Conclusion 119 1 Introduction and Statement Of The Resultsmentioning
confidence: 99%
“…5 The action (112) is covariant w.r.t. infinite-dimensional Lie algebra G which has the structure of a semidirect product of all canonical transformations with parameters ǫ(x, p)…”
Section: Classical Geometrymentioning
confidence: 99%
“…As mentioned in Introduction one reason for this is that the full spectrum of fields in the appropriate higher spin supermultiplet also contains spin 0, 1/2 and 1 massless fields not included in the consideration of this paper. Our modest goal here is to show that, similarly to the 4d case [16], the problem with (cubic) higher-spingravitational interactions in the flat background [30,31] can be avoided in AdS 5 .…”
Section: General Propertiesmentioning
confidence: 99%
“…Severe restrictions arise from powerful no-go theorems [1][2][3][4][5], which prohibit, in Minkowski space, minimal coupling to gravity, when the particle's spin s ≥ 5 2 , as well as to electromagnetism (EM), when s ≥ 3 2 . However, these particles may still interact through gravitational and EM multipoles.…”
Section: Jhep08(2012)093 1 Introductionmentioning
confidence: 99%
“…We do not consider mixed-symmetry fields, and restrict our attention to totally symmetric Dirac fermions ψ µ 1 ...µn , of spin s = n+ 1 2 . For these fields, we employ the powerful machinery of BRST-BV cohomological methods [20,21] to construct systematically consistent interaction vertices, 2 with the underlying assumptions of locality, Poincaré invariance and conservation of parity, and without relying on other methods. The would-be off-shell 1 − s − s cubic vertices will complement their bosonic counterparts constructed in [9].…”
Section: Jhep08(2012)093 1 Introductionmentioning
confidence: 99%