AdS3 solutions in massive IIA with small N $$ \mathcal{N} $$ = (4, 0) supersymmetry

Abstract We study AdS3 x S 2 solutions in massive IIA that preserve small N $$ \mathcal{N} $$ = (4, 0) supersymmetry in terms of an SU(2)-structure on the remaining internal space. We find two new classes of solutions that are warped products of the form AdS3 x S2 x M4 x ℝ. For the first, M4=CY2 and...

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Main Authors: Yolanda Lozano, Niall T. Macpherson, Carlos Nunez, Anayeli Ramirez
Format: Article
Language:English
Published: SpringerOpen 2020-01-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP01(2020)129
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author Yolanda Lozano
Niall T. Macpherson
Carlos Nunez
Anayeli Ramirez
author_facet Yolanda Lozano
Niall T. Macpherson
Carlos Nunez
Anayeli Ramirez
author_sort Yolanda Lozano
collection DOAJ
description Abstract We study AdS3 x S 2 solutions in massive IIA that preserve small N $$ \mathcal{N} $$ = (4, 0) supersymmetry in terms of an SU(2)-structure on the remaining internal space. We find two new classes of solutions that are warped products of the form AdS3 x S2 x M4 x ℝ. For the first, M4=CY2 and we find a generalisation of a D4-D8 system involving possible additional branes. For the second, M4 need only be Kahler, and we find a generalisation of the T-dual of solutions based on D3-branes wrapping curves in the base of an elliptically fibered Calabi-Yau 3-fold. Within these classes we find many new locally compact solutions that are foliations of AdS3 x S2 x CY2 over an interval, bounded by various D brane and O plane behaviours. We comment on how these local solutions may be used as the building blocks of infinite classes of global solutions glued together with defect branes. Utilising T-duality we find two new classes of AdS3 x S3 x M4 solutions in liB. The first backreacts D5s and KK monopoles on the D1-D5 near horizon. The second is a generalisation of the solutions based on D3-branes wrapping curves in the base of an elliptically fibered CY3 that includes non trivial 3-form flux.
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spelling doaj-art-cc973d1c08364d2eb2c4f61417f25b852025-01-26T12:11:31ZengSpringerOpenJournal of High Energy Physics1029-84792020-01-012020114310.1007/JHEP01(2020)129AdS3 solutions in massive IIA with small N $$ \mathcal{N} $$ = (4, 0) supersymmetryYolanda Lozano0Niall T. Macpherson1Carlos Nunez2Anayeli Ramirez3Department of Physics, University of OviedoSISSA International School for Advanced Studies and INFN sezione di TriesteDepartment of Physics, Swansea UniversityDepartment of Physics, University of OviedoAbstract We study AdS3 x S 2 solutions in massive IIA that preserve small N $$ \mathcal{N} $$ = (4, 0) supersymmetry in terms of an SU(2)-structure on the remaining internal space. We find two new classes of solutions that are warped products of the form AdS3 x S2 x M4 x ℝ. For the first, M4=CY2 and we find a generalisation of a D4-D8 system involving possible additional branes. For the second, M4 need only be Kahler, and we find a generalisation of the T-dual of solutions based on D3-branes wrapping curves in the base of an elliptically fibered Calabi-Yau 3-fold. Within these classes we find many new locally compact solutions that are foliations of AdS3 x S2 x CY2 over an interval, bounded by various D brane and O plane behaviours. We comment on how these local solutions may be used as the building blocks of infinite classes of global solutions glued together with defect branes. Utilising T-duality we find two new classes of AdS3 x S3 x M4 solutions in liB. The first backreacts D5s and KK monopoles on the D1-D5 near horizon. The second is a generalisation of the solutions based on D3-branes wrapping curves in the base of an elliptically fibered CY3 that includes non trivial 3-form flux.https://doi.org/10.1007/JHEP01(2020)129Extended SupersymmetrySupergravity ModelsAdS-CFT CorrespondenceD-branes
spellingShingle Yolanda Lozano
Niall T. Macpherson
Carlos Nunez
Anayeli Ramirez
AdS3 solutions in massive IIA with small N $$ \mathcal{N} $$ = (4, 0) supersymmetry
Journal of High Energy Physics
Extended Supersymmetry
Supergravity Models
AdS-CFT Correspondence
D-branes
title AdS3 solutions in massive IIA with small N $$ \mathcal{N} $$ = (4, 0) supersymmetry
title_full AdS3 solutions in massive IIA with small N $$ \mathcal{N} $$ = (4, 0) supersymmetry
title_fullStr AdS3 solutions in massive IIA with small N $$ \mathcal{N} $$ = (4, 0) supersymmetry
title_full_unstemmed AdS3 solutions in massive IIA with small N $$ \mathcal{N} $$ = (4, 0) supersymmetry
title_short AdS3 solutions in massive IIA with small N $$ \mathcal{N} $$ = (4, 0) supersymmetry
title_sort ads3 solutions in massive iia with small n mathcal n 4 0 supersymmetry
topic Extended Supersymmetry
Supergravity Models
AdS-CFT Correspondence
D-branes
url https://doi.org/10.1007/JHEP01(2020)129
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