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Hyper-Dilaton Weyl Multiplets of 5D and 6D Minimal Conformal Supergravity
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abstract
By extending the recent analysis of arXiv:2203.12203 for ${\mathcal{N}}=2$ conformal supergravity in four dimensions, we define new hyper-dilaton Weyl multiplets for five-dimensional ${\mathcal{N}}=1$, and six-dimensional ${\mathcal{N}}=(1,0)$ conformal supergravities. These are constructed by coupling the five- and six-dimensional standard Weyl multiplets to on-shell hypermultiplets and reinterpreting the systems as new multiplets of conformal supergravity. In the five-dimensional case, we also construct a new hyper-dilaton Poincar\'e supergravity by coupling to an off-shell vector multiplet compensator. As in four dimensions, a $BF$-coupling induces a non-trivial scalar potential for the five-dimensional dilaton that admits AdS$_5$ vacua.
Forward citations
Cited by 4 Pith papers
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Six-dimensional $\mathcal{N}=(2,0)$ Conformal Superspace
A new off-shell 6D N=(2,0) conformal superspace is constructed, and its unique Bach tensor superfield is derived up to overall scaling.
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$SU(2)\times SU(2)$ dilaton Weyl multiplets for maximal conformal supergravity in four, five, and six dimensions
New SU(2)×SU(2) dilaton Weyl multiplets are constructed for N=4, N=2, and (2,0) conformal supergravity, including the first six-dimensional (2,0) dilaton Weyl multiplet.
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${\mathcal N}=3$ nonlinear multiplet and supergravity
A new N=3 Einstein superspace is built from a proposed nonlinear multiplet, and the resulting equations of motion reduce to chi=0, implying the N=3 super-Bach tensor vanishes.
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Dilaton Weyl multiplets for $N = 3$ conformal supergravity in four dimensions
A dilaton Weyl multiplet for four-dimensional N=3 conformal supergravity is constructed in two versions, with R-symmetry SU(2)xU(1)xU(1) and then SU(2)xU(1).
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