Hyper-dilaton Weyl multiplet of 4D, $$ \mathcal{N} $$ = 2 conformal supergravity
We define a new dilaton Weyl multiplet of $$ \mathcal{N} $$ N = 2 conformal supergravity in four dimensions. This is constructed by reinterpreting the equations of motion of an on-shell hypermultiplet as constraints that render some of the fields of the standard Weyl multiplet composite. The indepen...
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Veröffentlicht in: | The journal of high energy physics 2022-09, Vol.2022 (9), Article 16 |
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Hauptverfasser: | , , , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | We define a new dilaton Weyl multiplet of
$$ \mathcal{N} $$
N
= 2 conformal supergravity in four dimensions. This is constructed by reinterpreting the equations of motion of an on-shell hypermultiplet as constraints that render some of the fields of the standard Weyl multiplet composite. The independent bosonic components include four scalar fields and a triplet of gauge two-forms. The resulting, so-called, hyper-dilaton Weyl multiplet defines a 24 + 24 off-shell representation of the local
$$ \mathcal{N} $$
N
= 2 superconformal algebra. By coupling the hyper-dilaton Weyl multiplet to an off-shell vector multiplet compensator, we obtain one of the two minimal 32 + 32 off-shell multiplets of
$$ \mathcal{N} $$
N
= 2 Poincaré supergravity constructed by Müller in 1986. On-shell, this contains the minimal
$$ \mathcal{N} $$
N
= 2 Poincaré supergravity multiplet together with a hypermultiplet where one of its physical scalars plays the role of a dilaton, while its three other scalars are dualised to a triplet of real gauge two-forms. Interestingly, a
BF
-coupling induces a scalar potential for the dilaton without a standard gauging. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP09(2022)016 |