2011
DOI: 10.1007/jhep10(2011)030
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$ \mathcal{N} = 2 $ conformal superspace in four dimensions

Abstract: Abstract:We develop the geometry of four dimensional N = 2 superspace where the entire conformal algebra of SU(2, 2|2) is realized linearly in the structure group rather than just the SL(2, C) × U(2) R subgroup of Lorentz and R-symmetries, extending to N = 2 our prior result for N = 1 superspace. This formulation explicitly lifts to superspace the existing methods of the N = 2 superconformal tensor calculus; at the same time the geometry, when degauged to SL(2, C) × U(2) R , reproduces the existing formulation… Show more

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Cited by 89 publications
(288 citation statements)
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“…Appendix A describes the component content of the nilpotent chiral scalar superfield Φ. Appendix B gives a summary of the SU(2) superspace [32], while appendix C briefly introduces N = 2 conformal superspace [33]. Finally, appendix D discusses nilpotent N = 1 supergravity following and extending [21].…”
Section: Jhep05(2017)061mentioning
confidence: 99%
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“…Appendix A describes the component content of the nilpotent chiral scalar superfield Φ. Appendix B gives a summary of the SU(2) superspace [32], while appendix C briefly introduces N = 2 conformal superspace [33]. Finally, appendix D discusses nilpotent N = 1 supergravity following and extending [21].…”
Section: Jhep05(2017)061mentioning
confidence: 99%
“…The three formulations prove to be equivalent, and they are also related to each other in the following sense: (i) SU(2) superspace is a gauged fixed version of U(2) superspace [59]; and (ii) U(2) superspace is a gauge fixed version of conformal superspace [33]. The most general off-shell N = 2 supergravity-matter couplings were constructed in SU(2) superspace [53,54], a few years before the conformal superspace was introduced.…”
Section: Two Realisations For the Chiral Goldstino Superfieldmentioning
confidence: 99%
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