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Mirrorfolds with K3 Fibrations
High Energy Physics - Theory · Submitted 7 Nov 2007
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Starting with arbitrary (compact or non-compact) Gepner models for the $K3$ fiber, we construct modular invariant partition functions of general mirrorfold models.
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The abstract, sentence by sentence
We study a class of non-geometric string vacua realized as completely soluble superconformal field theory (SCFT). These models are defined as `interpolating orbifolds' of $K3 \times S^1$ by the mirror transformation acting on the $K3$ fiber combined with the half-shift on the $S^1$-base. They are variants of the T-folds, the interpolating orbifolds by T-duality transformations, and thus may be called `mirrorfolds'. Starting with arbitrary (compact or non-compact) Gepner models for the $K3$ fiber, we construct modular invariant partition functions of general mirrorfold models. In the case of compact $K3$ fiber the mirrorfolds only yield non-supersymmetric string vacua. They exhibit IR instability due to winding tachyon condensation which is similar to the Scherk-Schwarz type circle compactification. When the fiber SCFT is non-compact (say, the ALE space in the simplest case), on the other hand, both supersymmetric and non-supersymmetric vacua can be constructed. The non-compact non-supersymmetric mirrorfolds can get stabilised at the level of string perturbation theory. We also find that in the non-compact supersymmeric mirrorfolds D-branes are {\em always} non-BPS. These D-branes can get stabilized against both open- and closed-string marginal deformations.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study a class of non-geometric string vacua realized as completely soluble superconformal field theory (SCFT). | contribution 1.00 | 0.91 | 0.10 | asserted 1.00 |
| s1 | These models are defined as `interpolating orbifolds' of $K3 \times S^1$ by the mirror transformation acting on the $K3$ fiber combined with the half-shift on the $S^1$-base. | method 0.61 | 0.49 | 0.08 | asserted 1.00 |
| s2 | They are variants of the T-folds, the interpolating orbifolds by T-duality transformations, and thus may be called `mirrorfolds'. | background 0.56 | 0.31 | 0.10 | hedged possibility 0.79 |
| s3 | Starting with arbitrary (compact or non-compact) Gepner models for the $K3$ fiber, we construct modular invariant partition functions of general mirrorfold models. | method 0.70 | 0.95 | 0.10 | asserted 1.00 |
| s4 | In the case of compact $K3$ fiber the mirrorfolds only yield non-supersymmetric string vacua. | result 0.98 | 0.82 | 0.12 | asserted 1.00 |
| s5 | They exhibit IR instability due to winding tachyon condensation which is similar to the Scherk-Schwarz type circle compactification. | result 0.95 | 0.80 | 0.09 | asserted 1.00 |
| s6 | When the fiber SCFT is non-compact (say, the ALE space in the simplest case), on the other hand, both supersymmetric and non-supersymmetric vacua can be constructed. | result 0.99 | 0.85 | 0.14 | asserted 0.81 |
| s7 | The non-compact non-supersymmetric mirrorfolds can get stabilised at the level of string perturbation theory. | result 1.00 | 0.82 | 0.12 | hedged possibility 0.78 |
| s8 | We also find that in the non-compact supersymmeric mirrorfolds D-branes are {\em always} non-BPS. | result 1.00 | 0.92 | 0.13 | asserted 1.00 |
| s9 | These D-branes can get stabilized against both open- and closed-string marginal deformations. | result 1.00 | 0.87 | 0.12 | asserted 0.76 |
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The paper
Original abstract
We study a class of non-geometric string vacua realized as completely soluble superconformal field theory (SCFT). These models are defined as `interpolating orbifolds' of $K3 \times S^1$ by the mirror transformation acting on the $K3$ fiber combined with the half-shift on the $S^1$-base. They are variants of the T-folds, the interpolating orbifolds by T-duality transformations, and thus may be called `mirrorfolds'. Starting with arbitrary (compact or non-compact) Gepner models for the $K3$ fiber, we construct modular invariant partition functions of general mirrorfold models. In the case of compact $K3$ fiber the mirrorfolds only yield non-supersymmetric string vacua. They exhibit IR instability due to winding tachyon condensation which is similar to the Scherk-Schwarz type circle compactification. When the fiber SCFT is non-compact (say, the ALE space in the simplest case), on the other hand, both supersymmetric and non-supersymmetric vacua can be constructed. The non-compact non-supersymmetric mirrorfolds can get stabilised at the level of string perturbation theory. We also find that in the non-compact supersymmeric mirrorfolds D-branes are {\em always} non-BPS. These D-branes can get stabilized against both open- and closed-string marginal deformations.
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References
How the literature uses it
14 arXiv papers cite this in 22 sentences
Papers citing it · 10 sentences without a confident label
Builds on it 1 paper
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The idea of T-folds can be naturally extended to compactifications with U-duality twists (U-folds) [ref] and, given the understanding of mirror symmetry as T-duality [ref] , may allow mirror-folds for Calabi-Yau compactifications [ref] .
T-duality Invariant Approaches to String Theory · T-folds · 0.82
Uses its method or tool 1 paper
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We can determine them in a way parallel to that presented in [ref] .
Non-supersymmetric D-branes with Vanishing Cylinder Amplitudes in Asymmetric Orbifolds · Concrete Examples : Gepner Construction · 0.98
Compares with it 1 paper
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Previously Kawai et Sugawara have considered in [ref] K3 mirror-folds with monodromies that, at least when the fiber is compact, break all supersymmetry; in the present work, we consider in contrast monodromies that preserve 8 supersymmetries, i.e. which preserve a quarter of the 32 supersymmetries of the type IIA string, or a half of the 16 supersymmetries of type IIA compactified on $K3$.
Non-geometric Calabi-Yau Backgrounds and K3 automorphisms · Introduction · 0.93
Cites it as background 7 papers
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The idea of a Mirror-fold is not new (see, for example, [ref] ) and in [ref] a CFT for the interpolating orbifold corresponding to a Mirror-fold was explicitly constructed.
N=4 Gauged Supergravity from Duality-Twist Compactifications of String Theory · Mirror-folds and Non-Geometric Backgrounds with $𝒬_i^A$ Flux · 0.92
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Such T-fold CFTs have been studied e.g. in [ref] .
Lie algebra lattices and strings on T-folds · Introduction · 0.86
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To our knowledge, analogous supersymmetric constructions in type IIA/IIB superstrings have not been considered yet.[Different constructions of non-supersymmetric asymmetric models were considered in [ref] .]
Asymmetric Gepner models in type II · Introduction · 0.81
What it cites · 36 sentences without a confident label
Uses the method or tool of 1 paper
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A way to circumvent this problem is to focus only on the propagating degrees of freedom, by considering the partition function per unit volume as discussed in [ref] ; [equation] Note that the second term $Z_dis$ drops after divided by the infinite volume factor $V$.
SL(2,R)/U(1) Supercoset and Elliptic Genera of Non-compact Calabi-Yau Manifolds · Non-SUSY Vacua : Symmetric Modular Invariants · 0.92
Cites as background 5 papers
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In such models the moduli space of the fibre, when going around non-trivial cycles on the base manifold, picks up monodromies in general; for this reason these string vacua are often called `monodrofolds.' In particular, monodrofolds constructed from T-duality transformations are called `T-folds' [ref] .
A Geometry for Non-Geometric String Backgrounds · Introduction and Summary · 0.98
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By now, several models of T-folds have been analysed using CFT [ref] .
Nongeometry, Duality Twists, and the Worldsheet · Introduction and Summary · 0.85
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By now, several models of T-folds have been analysed using CFT [ref] .
Worldsheet CFTs for Flat Monodrofolds · Introduction and Summary · 0.85
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