4.4 Article

Wrapped M5-branes, consistent truncations and AdS/CMT

Journal

JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 12, Pages -

Publisher

SPRINGER
DOI: 10.1007/JHEP12(2010)003

Keywords

Holography and condensed matter physics (AdS/CMT); Black Holes in String Theory; AdS-CFT Correspondence; M-Theory

Funding

  1. EPSRC
  2. Royal Society
  3. Korea government (MEST) [2009-0085995]
  4. Center for Quantum Spacetime (CQUeST) of Sogang University [2005-0049409]
  5. Alexander von Humboldt
  6. Spanish Government [FIS2008-01980]
  7. INFN
  8. Engineering and Physical Sciences Research Council [EP/D072077/1, EP/G050015/1] Funding Source: researchfish
  9. Science and Technology Facilities Council [ST/G000743/1] Funding Source: researchfish
  10. National Research Foundation of Korea [2010-0008082] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)
  11. EPSRC [EP/G050015/1, EP/D072077/1] Funding Source: UKRI
  12. STFC [ST/G000743/1] Funding Source: UKRI

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At the level of the bosonic fields, we construct consistent Kaluza-Klein reductions of D = 11 supergravity on Sigma(3) x S-4, where Sigma(3) = H-3/Gamma, S-3/Gamma or R-3/Gamma where Gamma is a discrete group of isometries. The result is the bosonic content of an N = 2 D = 4 gauged supergravity with a single vector multiplet and two hypermultiplets, whose scalar fields parametrise SU(1, 1)/U(1) x G(2(2))/SO(4). When Sigma(3) = H-3/Gamma the D = 4 theory has an AdS(4) vacuum which uplifts to the known supersymmetric AdS(4) x H-3/Gamma x S-4 solution of D = 11 supergravity that describes the N = 2 d = 3 SCFT arising when M5-branes wrap SLag 3-cycles H-3/Gamma in Calabi-Yau three-folds. We use the KK reduction for Sigma(3) = H-3/Gamma to construct D = 11 black hole solutions that describe these d = 3 SCFTs at finite temperature and charge density and show that there is a superconducting instability involving a charged scalar field, and another instability involving neutral fields including both scalar and vector fields. We also use this KK reduction to construct a D = 11 Lifshitz solution that is dual to a d = 3 field theory with dynamical exponent z similar to 39.

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