Abstract:We compute the new supersymmetric index of a large class of N=2 heterotic
compactifications with torsion, corresponding to principal two-torus bundles
over warped K3 surfaces with H-flux. Starting from a UV description as a (0,2)
gauged linear sigma-model with torsion, we use supersymmetric localization
techniques to provide an explicit expression of the index as a sum over the
Jeffrey-Kirwan residues of the one-loop determinant. We finally propose a
geometrical formula that gives the new supersymmetric index … Show more
“…The result is that such a gauge theory may a priori correspond to several distinct SCFTs, labelled by the choice of branch. 6 In addition, there are also a number of interesting examples of (2, 2) and (0, 2) abelian gauge theories with dynamical Fayet-Iliopoulos and θ-angle terms, for instance references [69][70][71][72][73][74].…”
Compactifications of 6D superconformal field theories (SCFTs) on four-manifolds generate a large class of novel 2d quantum field theories. We consider in detail the case of the rank one simple non-Higgsable cluster 6D SCFTs. On the tensor branch of these theories, the gauge group is simple and there are no matter fields. For compactifications on suitably chosen Kähler surfaces, we present evidence that this provides a method to realize 2d SCFTs with N = (0, 2) supersymmetry. In particular, we find that reduction on the tensor branch of the 6D SCFT yields a description of the same 2d fixed point that is described in the UV by a gauged linear sigma model (GLSM) in which the parameters are promoted to dynamical fields, that is, a "dynamic GLSM" (DGLSM). Consistency of the model requires the DGLSM to be coupled to additional non-Lagrangian sectors obtained from reduction of the anti-chiral two-form of the 6D theory. These extra sectors include both chiral and anti-chiral currents, as well as spacetime filling non-critical strings of the 6D theory. For each candidate 2d SCFT, we also extract the left-and right-moving central charges in terms of data of the 6D SCFT and the compactification manifold. *
“…The result is that such a gauge theory may a priori correspond to several distinct SCFTs, labelled by the choice of branch. 6 In addition, there are also a number of interesting examples of (2, 2) and (0, 2) abelian gauge theories with dynamical Fayet-Iliopoulos and θ-angle terms, for instance references [69][70][71][72][73][74].…”
Compactifications of 6D superconformal field theories (SCFTs) on four-manifolds generate a large class of novel 2d quantum field theories. We consider in detail the case of the rank one simple non-Higgsable cluster 6D SCFTs. On the tensor branch of these theories, the gauge group is simple and there are no matter fields. For compactifications on suitably chosen Kähler surfaces, we present evidence that this provides a method to realize 2d SCFTs with N = (0, 2) supersymmetry. In particular, we find that reduction on the tensor branch of the 6D SCFT yields a description of the same 2d fixed point that is described in the UV by a gauged linear sigma model (GLSM) in which the parameters are promoted to dynamical fields, that is, a "dynamic GLSM" (DGLSM). Consistency of the model requires the DGLSM to be coupled to additional non-Lagrangian sectors obtained from reduction of the anti-chiral two-form of the 6D theory. These extra sectors include both chiral and anti-chiral currents, as well as spacetime filling non-critical strings of the 6D theory. For each candidate 2d SCFT, we also extract the left-and right-moving central charges in terms of data of the 6D SCFT and the compactification manifold. *
“…In this work, we have computed the one-loop threshold corrections to the gauge and gravitational couplings in a large class of N = 2 heterotic compactifications on non-Kähler manifolds with three-form flux. We have obtained the result from the new supersymmetric index that was computed in [10,11].…”
Section: Resultsmentioning
confidence: 99%
“…For the N = 2 torsional compactifications of interest, the new supersymmetric index was computed in [10], using a purposely designed gauged linear sigma model [7] and supersymmetric localization of the path integral [32]. A main difference with the conventional K3 × T 2 compactifications is that both the complex structure and complexified Kähler moduli of the two-torus fiber are now generically quantized.…”
Section: N = Heterotic Threshold Corrections and The New Supersymmetrmentioning
confidence: 99%
“…The new supersymmetric index (2.3) was then computed in terms of this data in [10,11]. First, the dressed elliptic genus (2.6) can be written as a sum of three terms in the following way:…”
Section: N = Heterotic Threshold Corrections and The New Supersymmetrmentioning
confidence: 99%
“…Localization techniques were then used by two of the present authors to compute the new supersymmetric index [10,11], which is, in the context of heterotic N = 2 compactifications, the building block that is used to compute the threshold corrections to the BPS-saturated couplings in the low energy four-dimensional N = 2 supergravity action [12].…”
Abstract:We compute the one-loop threshold corrections to the gauge and gravitational couplings for a large class of N = 2 non-Kähler heterotic compactifications with three-form flux, consisting in principal two-torus bundles over K3 surfaces. We obtain the results as sums of BPS-states contributions, depending on the topological data of the bundle. We analyse also the worldsheet non-perturbative corrections coming from instantons wrapping the torus fiber, that are mapped under S-duality to D-instanton corrections in type I flux compactifications.
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