Abstract:We study aspects of superstring vacua of non-compact special holonomy manifolds with conical singularities constructed systematically using soluble N = 1 superconformal field theories (SCFT's). It is known that Einstein homogeneous spaces G/H generate Ricci flat manifolds with special holonomies on their cones ≃ R + × G/H, when they are endowed with appropriate geometrical structures, namely, the Sasaki-Einstein, triSasakian, nearly Kähler, and weak G 2 structures for SU(n), Sp(n), G 2 , and Spin (7) holonomie… Show more
“…Mirror symmetry of the flux backgrounds should then induce mirror symmetry of these G 2 manifolds. Finally, it would be interesting to study this mirror symmetry for other G 2 manifolds for which a conformal field theory description is available [13,[22][23][24][25][26][27][28]. It may also be interesting to see whether there is a similar construction for Spin(8) manifolds.…”
A generalisation of discrete torsion is introduced in which different discrete torsion phases are considered for the different fixed points or twist fields of a twisted sector. The constraints that arise from modular invariance are analysed carefully. As an application we show how all the different resolutions of the T 7 /Z 3 2 orbifold of Joyce have an interpretation in terms of such generalised discrete torsion orbifolds. Furthermore, we show that these manifolds are pairwise identified under G 2 mirror symmetry. From a conformal field theory point of view, this mirror symmetry arises from an automorphism of the extended chiral algebra of the G 2 compactification.
“…Mirror symmetry of the flux backgrounds should then induce mirror symmetry of these G 2 manifolds. Finally, it would be interesting to study this mirror symmetry for other G 2 manifolds for which a conformal field theory description is available [13,[22][23][24][25][26][27][28]. It may also be interesting to see whether there is a similar construction for Spin(8) manifolds.…”
A generalisation of discrete torsion is introduced in which different discrete torsion phases are considered for the different fixed points or twist fields of a twisted sector. The constraints that arise from modular invariance are analysed carefully. As an application we show how all the different resolutions of the T 7 /Z 3 2 orbifold of Joyce have an interpretation in terms of such generalised discrete torsion orbifolds. Furthermore, we show that these manifolds are pairwise identified under G 2 mirror symmetry. From a conformal field theory point of view, this mirror symmetry arises from an automorphism of the extended chiral algebra of the G 2 compactification.
“…It is also perhaps worthwhile to investigate more concrete world-sheet models of theories based on the G 2 algebra, for example using minimal models and discrete torsion, see e.g. [15,16,17,18,19,20,21,22,23]. It is also interesting to extend this construction to more general setting which involve turning on the NS-NS background fields.…”
Section: Open Problems and Future Directionsmentioning
confidence: 99%
“…For more about type II strings on G 2 manifolds and their mirror symmetry, see e.g. [13,14,15,16,17,18,19,20,21,22,23]. A review of M-theory on G 2 manifolds with many references can be found in [24].…”
We construct new topological theories related to sigma models whose target space is a seven dimensional manifold of G 2 holonomy. We define a new type of topological twist and identify the BRST operator and the physical states. Unlike the more familiar six dimensional case, our topological model is defined in terms of conformal blocks and not in terms of local operators of the original theory. We also present evidence that one can extend this definition to all genera and construct a seven-dimensional topological string theory. We compute genus zero correlation functions and relate these to Hitchin's functional for three-forms in seven dimensions. Along the way we develop the analogue of special geometry for G 2 manifolds. When the seven dimensional topological twist is applied to the product of a Calabi-Yau manifold and a circle, the result is an interesting combination of the six dimensional A-and B-models.
“…Recently, the work in ref. [27] implies that if the SCFT N contains a tri-critical Ising model, then N = 1 supersymmetry can be constructed in the boundary dual of AdS 3 . A new family of examples of this sort is N = SO(7) k ′ /(G 2 ) k ′ +1 , which leads to precisely N = 1 two dimensional supersymmetry in spacetime 13 .…”
We study superstring theories on AdS 3 × N backgrounds yielding N = 2, 3, 4 extended superconformal symmetries in the dual boundary CFT. In each case the necessary constraints on the internal worldsheet theory N are found. 15 4. Spacetime small and large N = 4 supersymmetry 16 5. Discussion 17 A. Properties of the affine currents 18 B. Realization of the symmetries for N = 3 19
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