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K-K excitations on $AdS_{5} \times S^{5}$ as $N=4$ "primary" superfields

We show that the K-K spectrum of IIB string on AdS_5 x S_5 is described by ``twisted chiral'' N=4 superfields, naturally described in ``harmonic superspace'', obtained by taking suitable gauge singlets polynomials of the D3-brane boundary SU(n) superconformal field theory. To eac...

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Detalles Bibliográficos
Autores principales: Andrianopoli, L., Ferrara, S.
Lenguaje:eng
Publicado: 1998
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(98)00553-X
http://cds.cern.ch/record/349672
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author Andrianopoli, L.
Ferrara, S.
author_facet Andrianopoli, L.
Ferrara, S.
author_sort Andrianopoli, L.
collection CERN
description We show that the K-K spectrum of IIB string on AdS_5 x S_5 is described by ``twisted chiral'' N=4 superfields, naturally described in ``harmonic superspace'', obtained by taking suitable gauge singlets polynomials of the D3-brane boundary SU(n) superconformal field theory. To each p-order polynomial is associated a massive K-K short representation with 256 x 1/12 p^2(p^2 -1) states. The p=2 quadratic polynomial corresponds to the ``supercurrent multiplet'' describing the ``massless'' bulk graviton multiplet.
id cern-349672
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1998
record_format invenio
spelling cern-3496722023-03-14T19:52:00Zdoi:10.1016/S0370-2693(98)00553-Xhttp://cds.cern.ch/record/349672engAndrianopoli, L.Ferrara, S.K-K excitations on $AdS_{5} \times S^{5}$ as $N=4$ "primary" superfieldsParticle Physics - TheoryWe show that the K-K spectrum of IIB string on AdS_5 x S_5 is described by ``twisted chiral'' N=4 superfields, naturally described in ``harmonic superspace'', obtained by taking suitable gauge singlets polynomials of the D3-brane boundary SU(n) superconformal field theory. To each p-order polynomial is associated a massive K-K short representation with 256 x 1/12 p^2(p^2 -1) states. The p=2 quadratic polynomial corresponds to the ``supercurrent multiplet'' describing the ``massless'' bulk graviton multiplet.We show that the K-K spectrum of IIB string on AdS_5 x S_5 is described by ``twisted chiral'' N=4 superfields, naturally described in ``harmonic superspace'', obtained by taking suitable gauge singlets polynomials of the D3-brane boundary SU(n) superconformal field theory. To each p-order polynomial is associated a massive K-K short representation with 256 x 1/12 p^2(p^2 -1) states. The p=2 quadratic polynomial corresponds to the ``supercurrent multiplet'' describing the ``massless'' bulk graviton multiplet.We show that the K–K spectrum of IIB string on AdS 5 × S 5 is described by “twisted chiral” N =4 superfields, naturally described in “harmonic superspace”, obtained by taking suitable gauge singlets polynomials of the D 3-brane boundary SU ( n ) superconformal field theory.hep-th/9803171CERN-TH-98-91CERN-TH-98-091oai:cds.cern.ch:3496721998-03-23
spellingShingle Particle Physics - Theory
Andrianopoli, L.
Ferrara, S.
K-K excitations on $AdS_{5} \times S^{5}$ as $N=4$ "primary" superfields
title K-K excitations on $AdS_{5} \times S^{5}$ as $N=4$ "primary" superfields
title_full K-K excitations on $AdS_{5} \times S^{5}$ as $N=4$ "primary" superfields
title_fullStr K-K excitations on $AdS_{5} \times S^{5}$ as $N=4$ "primary" superfields
title_full_unstemmed K-K excitations on $AdS_{5} \times S^{5}$ as $N=4$ "primary" superfields
title_short K-K excitations on $AdS_{5} \times S^{5}$ as $N=4$ "primary" superfields
title_sort k-k excitations on $ads_{5} \times s^{5}$ as $n=4$ "primary" superfields
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/S0370-2693(98)00553-X
http://cds.cern.ch/record/349672
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