Abstract

It is well known that Hopf-fibre T-duality and uplift takes the D1-D5 near-horizon into a class of $AdS_3 \times S^2$ geometries in 11D where the internal space is a Calabi-Yau three-fold. Moreover, supersymmetry dictates that Calabi-Yau is the only permissible $SU(3)$-structure manifold. Generalising this duality chain to non-Abelian isometries, a strong parallel exists, resulting in the first explicit example of a class of $AdS_3 \times S^2$ geometries with $SU(2)$-structure. Furthermore, the non-Abelian T-dual of $AdS_3 \times S^3 \times S^3 \times S^1$ results in a new supersymmetric $AdS_3 \times S^2$ geometry, which falls outside of all known classifications. We explore the basic properties of the holographic duals associated to the new backgrounds. We compute the central charges and show that they are compatible with a large $\mathcal{N}=4$ superconformal algebra in the infra-red.

Highlights

  • Applying the general rules in [66] we find a dual metric L2ds2(AdS3) R+2 ds2(S+3 ) 4 R−2 R−6 ρ2 64∆dχ2 + sin2 χdξ2 where ∆ R−6 16R−2 ρ2 64+ dx2, (4.1) (4.2)The dual dilaton is given by e−2Φ = ∆, while the NS 2-form is

  • By analyzing the same brane configurations we argue that the field theory dual shares some common properties with the CFT dual to the original AdS3 × S3 × S3 × S1 background but in a less symmetric fashion

  • We show that the solutions constructed through non-Abelian T-duality from the AdS3 × S3 × S3 × S1 background exhibit large N = (0, 4) supersymmetry

Read more

Summary

Quantized charges

The transformation of the RR fluxes under non-Abelian T-duality implies that the D1 color branes of the original background transform into D2-branes extended on {t, x1, ρ} and D4branes on {t, x1, ρ, S2}. We show that there are quantized charges in the non-Abelian T-dual background that can be associated to these branes

Instantons
Baryon vertices and ’t Hooft monopoles
Central charge
Background
Large gauge transformations
Color branes
Flavor branes
A possible brane intersection?
Baryon vertices and t’Hooft monopoles
Comments on supersymmetry
Conclusions
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.