Spectrum of D = 6, N = 4b supergravity on AdS3 × S3

S. Deger, A. Kaya, E. Sezgin, P. Sundell

Resultado de la investigación: Article

102 Citas (Scopus)

Resumen

The complete spectrum of D = 6, N = 4b supergravity with n tensor multiplets compactified on AdS3 × S3 is determined. The D = 6 theory obtained from the K3 compactification of Type IIB string requires that n = 21, but we let n be arbitrary. The superalgebra that underlies the symmetry of the resulting supergravity theory in AdS3 coupled to matter is SU(1, 1|2)L × SU(1, 1|2)R. The theory also has an unbroken global SO(4)R × SO(n) symmetry inherited from D = 6. The spectrum of states arranges itself into a tower of spin-2 supermultiplets, a tower of spin-1, SO(n) singlet supermultiplets, a tower of spin-1 supermultiplets in the vector representation of SO(n) and a special spin-1/2 supermultiplet also in the vector representation of SO(n). The SU(2)L × SU(2)R Yang-Mills states reside in the second level of the spin-2 tower and the lowest level of the spin-1, SO(n) singlet tower and the associated field theory exhibits interesting properties.

Idioma originalEnglish
Páginas (desde-hasta)110-140
Número de páginas31
PublicaciónNuclear Physics B
Volumen536
N.º1-2
DOI
EstadoPublished - 21 dic 1998

Huella dactilar

supergravity
towers
symmetry
strings
fine structure
tensors

ASJC Scopus subject areas

  • Nuclear and High Energy Physics

Citar esto

Deger, S. ; Kaya, A. ; Sezgin, E. ; Sundell, P. / Spectrum of D = 6, N = 4b supergravity on AdS3 × S3 En: Nuclear Physics B. 1998 ; Vol. 536, N.º 1-2. pp. 110-140.
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Spectrum of D = 6, N = 4b supergravity on AdS3 × S3 . / Deger, S.; Kaya, A.; Sezgin, E.; Sundell, P.

En: Nuclear Physics B, Vol. 536, N.º 1-2, 21.12.1998, p. 110-140.

Resultado de la investigación: Article

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AU - Sundell, P.

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AB - The complete spectrum of D = 6, N = 4b supergravity with n tensor multiplets compactified on AdS3 × S3 is determined. The D = 6 theory obtained from the K3 compactification of Type IIB string requires that n = 21, but we let n be arbitrary. The superalgebra that underlies the symmetry of the resulting supergravity theory in AdS3 coupled to matter is SU(1, 1|2)L × SU(1, 1|2)R. The theory also has an unbroken global SO(4)R × SO(n) symmetry inherited from D = 6. The spectrum of states arranges itself into a tower of spin-2 supermultiplets, a tower of spin-1, SO(n) singlet supermultiplets, a tower of spin-1 supermultiplets in the vector representation of SO(n) and a special spin-1/2 supermultiplet also in the vector representation of SO(n). The SU(2)L × SU(2)R Yang-Mills states reside in the second level of the spin-2 tower and the lowest level of the spin-1, SO(n) singlet tower and the associated field theory exhibits interesting properties.

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