2018
DOI: 10.1016/j.physletb.2018.01.045
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Non-conformal higher spin supercurrents

Abstract: In four spacetime dimensions there exist two off-shell formulations for the massless multiplet of superspin (s + 1 2 ), where s = 2, 3, . . . . These supersymmetric higher spin gauge theories, known as longitudinal and transverse, are dual to each other and describe two massless fields of spin (s + 1 2 ) and (s + 1) upon elimination of the auxiliary fields. They respectively reduce, in the limiting case of s = 1, to the linearised actions for the old minimal and the n = −1 non-minimal N = 1 supergravity theori… Show more

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Cited by 33 publications
(38 citation statements)
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References 37 publications
(48 reference statements)
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“…The result of that would be that, the spectrum of the half integer supermultiplet will collapse from (s + 1, s + 1/2, s + 1/2, s) to (s + 1, s + 1/2) and more importantly the generator of cubic interactions J α(s)α(s) in (18) will become conserved higher spin supercurrents. Such supercurrents have been found in [68][69][70][71][72][73][74][75][76] and their structure is consistent with (20). are explicitly after in this work.…”
Section: Supersymmetric Higher Spinssupporting
confidence: 85%
“…The result of that would be that, the spectrum of the half integer supermultiplet will collapse from (s + 1, s + 1/2, s + 1/2, s) to (s + 1, s + 1/2) and more importantly the generator of cubic interactions J α(s)α(s) in (18) will become conserved higher spin supercurrents. Such supercurrents have been found in [68][69][70][71][72][73][74][75][76] and their structure is consistent with (20). are explicitly after in this work.…”
Section: Supersymmetric Higher Spinssupporting
confidence: 85%
“…Massless models given in this section will serve as the building blocks for our construction of the massive was considered in [12]. The superfield approach was recently applied for construction of the higher spin supercurrents [13], [14], [15]. [16], [17], [18], [19].…”
Section: Introductionmentioning
confidence: 99%
“…• General non-conformal deformations of the conformal supercurrents J α(n)α(n) and J α(n+1)α(n) , eq. (4.15), were described in [64,100,101] for the cases of Minkowski and AdS backgrounds. Various aspects of such non-conformal higher-spin supercurrents in Minkowski superspace were studied in [102][103][104].…”
Section: Resultsmentioning
confidence: 99%