TY - JOUR
T1 - Unitary supermultiplets of OSp(8*|4) and the AdS7/CFT6 duality
AU - Günaydin, Murat
AU - Takemae, Seiji
N1 - Funding Information:
I Work supported in part by the National Science Foundation under Grant Number PHY-9802510. ∗ [email protected] 1 [email protected]
PY - 2000/7/3
Y1 - 2000/7/3
N2 - We study the unitary supermultiplets of the N=4d=7 anti-de Sitter ( AdS7 ) superalgebra OSp(8*|4) , with the even subalgebra SO(6,2)×USp(4) , which is the symmetry superalgebra of M-theory on AdS7×S4 . We give a complete classification of the positive energy doubleton and massless supermultiplets of OSp(8*|4) . The ultra-short doubleton supermultiplets do not have the Poincaré limit in AdS7 and correspond to superconformal field theories on the boundary of AdS7 which can be identified with d=6 Minkowski space. We show that the six-dimensional Poincaré mass operator m2=PμPμ vanishes identically for the doubleton representations. By going from the compact U(4) basis of SO*(8)=SO(6,2) to the noncompact basis SU*(4)×D (d=6 Lorentz group times dilatations) one can associate the positive (conformal) energy representations of SO*(8) with conformal fields transforming covariantly under the Lorentz group in d=6 . The oscillator method used for the construction of the unitary supermultiplets of OSp(8*|4) can be given a dynamical realization in terms of chiral super-twistor fields.
AB - We study the unitary supermultiplets of the N=4d=7 anti-de Sitter ( AdS7 ) superalgebra OSp(8*|4) , with the even subalgebra SO(6,2)×USp(4) , which is the symmetry superalgebra of M-theory on AdS7×S4 . We give a complete classification of the positive energy doubleton and massless supermultiplets of OSp(8*|4) . The ultra-short doubleton supermultiplets do not have the Poincaré limit in AdS7 and correspond to superconformal field theories on the boundary of AdS7 which can be identified with d=6 Minkowski space. We show that the six-dimensional Poincaré mass operator m2=PμPμ vanishes identically for the doubleton representations. By going from the compact U(4) basis of SO*(8)=SO(6,2) to the noncompact basis SU*(4)×D (d=6 Lorentz group times dilatations) one can associate the positive (conformal) energy representations of SO*(8) with conformal fields transforming covariantly under the Lorentz group in d=6 . The oscillator method used for the construction of the unitary supermultiplets of OSp(8*|4) can be given a dynamical realization in terms of chiral super-twistor fields.
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U2 - 10.1016/S0550-3213(00)00026-2
DO - 10.1016/S0550-3213(00)00026-2
M3 - Article
AN - SCOPUS:0034600578
SN - 0550-3213
VL - 578
SP - 405
EP - 448
JO - Nuclear Physics B
JF - Nuclear Physics B
IS - 1-2
ER -