2006
DOI: 10.1016/j.nuclphysb.2006.04.018
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Classification of supersymmetric flux vacua in M-theory

Abstract: We present a comprehensive classification of supersymmetric vacua of M-theory compactification on seven-dimensional manifolds with general four-form fluxes. We analyze the cases where the resulting four-dimensional vacua have N = 1,2,3,4 supersymmetry and the internal space allows for SU (2), SU (3) or G 2 structures. In particular, we find for N = 2 supersymmetry, that the external space-time is Minkowski and the base manifold of the internal space is conformally Kähler for SU (2) structures, while for SU (3)… Show more

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Cited by 40 publications
(71 citation statements)
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“…In addition to that, the coefficients α 5,6 and β 5,6 have the same equivalence relations as in (2.34), although − and this is very crucial − α 3,4 and β 3,4 are no longer related by (2.34) because of the back-reactions of the B-fields. The coefficients γ 5,6 are expected to satisfy the following approximate relation…”
Section: Supergravity Solution Without Branesmentioning
confidence: 89%
“…In addition to that, the coefficients α 5,6 and β 5,6 have the same equivalence relations as in (2.34), although − and this is very crucial − α 3,4 and β 3,4 are no longer related by (2.34) because of the back-reactions of the B-fields. The coefficients γ 5,6 are expected to satisfy the following approximate relation…”
Section: Supergravity Solution Without Branesmentioning
confidence: 89%
“…Moreover, since the three-cycles intersect pair-wise, the massless chiral matters appear at these intersections. This construction [27] therefore provides an explicit example of supersymmetric flux compactifications with intersecting D6-branes. Further progress has also been made in the construction of N = 1 supersymmetric Type IIA flux vacua with SU(2) structures [27], leading to examples with the internal space conformally Calabi-Yau.…”
Section: Introductionmentioning
confidence: 96%
“…This construction [27] therefore provides an explicit example of supersymmetric flux compactifications with intersecting D6-branes. Further progress has also been made in the construction of N = 1 supersymmetric Type IIA flux vacua with SU(2) structures [27], leading to examples with the internal space conformally Calabi-Yau. However, explicit constructions of models with intersecting probe D6-branes for such flux compactifications is still awaiting further study.…”
Section: Introductionmentioning
confidence: 96%
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“…Seperately, various classes of supersymmetric AdS spacetimes in M-theory have been classified, by inserting an appropriately general AdS ansatz directly into the Killing spinor equation of eleven dimensional supergravity; minimally supersymmetric AdS 3 in [35], minimal purely magnetic AdS 4 in [38] and minimal AdS 5 in [39]. Some refinements of these AdS classifications have also appeared; for AdS 4 in [40] and AdS 5 with N = 2 supersymmetry in [41].…”
Section: Introductionmentioning
confidence: 99%