2000
DOI: 10.1016/s0550-3213(00)00026-2
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Unitary supermultiplets of and the AdS7/CFT6 duality

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Cited by 31 publications
(35 citation statements)
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“…In [18] it was shown explicitly how to go from the compact U(4) particle basis of the ULWR's of SO * (8) to the non-compact SU * (4) × SO(1, 1) coherent state basis. ( SU * (4) × SO(1, 1) is simply the covering group of the Lorentz group in six dimensions times dilatations) .…”
Section: Covariant Quantum Fields Over Generalized Spacetimes and Thementioning
confidence: 99%
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“…In [18] it was shown explicitly how to go from the compact U(4) particle basis of the ULWR's of SO * (8) to the non-compact SU * (4) × SO(1, 1) coherent state basis. ( SU * (4) × SO(1, 1) is simply the covering group of the Lorentz group in six dimensions times dilatations) .…”
Section: Covariant Quantum Fields Over Generalized Spacetimes and Thementioning
confidence: 99%
“…As was done explicitly for the conformal groups in 4 and 6 dimensions [17,18] one can show that there exists a rotation operator W in the representation space with the property that the states W |Ω are annihilated by all the generators belonging to n − n − W |Ω = 0…”
Section: Covariant Quantum Fields Over Generalized Spacetimes and Thementioning
confidence: 99%
“…Similarly, the conformal group SO * (8) of the Jordan algebra J H 2 parametrizing the six dimensional Minkowski space has a maximal compact subgroup U(4) which is the compact form of the structure group SU * (4) × SO(1, 1). In [22] it was shown how to go from the compact U(4) basis of the ULWR's of SO * (8) to the non-compact basis SU * (4) × SO(1, 1) which is simply the Lorentz group in six dimensions times dilatations. The coherent states of the non-compact basis are again labelled by the elements of the Jordan algebra J H 2 of 2×2 hermitian quaternionic matrices representing the coordinates of 6d Minkowski space.…”
Section: Conformal Fields Over Generalized Spacetimes and The Positivmentioning
confidence: 99%
“…These representations have been called " doubletons" since they require two sets of oscillators for their realization [10,12]. The doubleton supermultiplets of extended AdS supergroups in d = 5 (SU(2, 2/N)) and d = 7 (OSp(8 * /2N)) share the same remarkable features of the singleton supermultiplets of d = 4 AdS supergroups i.e the tensor product of any two doubletons decompose into an infinite set of massless supermultiplets [10,12,19,20,21,22]. In d = 3 the AdS group SO(2, 2) is not simple and is isomorphic to SO(2, 1) × SO(2, 1).…”
mentioning
confidence: 99%
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