2013
DOI: 10.1007/jhep02(2013)017
|View full text |Cite
|
Sign up to set email alerts
|

Ground states of duality-twisted sigma-models with K 3 target space

Abstract: We analyze the ground states of a two-dimensional sigma-model whose target space is an elliptically fibered K 3 , with the sigma-model compactified on S 1 with boundary conditions twisted by a duality symmetry. We show that the Witten index receives contributions from two kinds of states: (i) those that can be mapped to cohomology with coefficients in a certain line bundle over the target space, and (ii) states whose wavefunctions are localized at singular fibers. We also discuss the orbifold limit and possibl… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
3
0

Year Published

2015
2015
2021
2021

Publication Types

Select...
3

Relationship

1
2

Authors

Journals

citations
Cited by 3 publications
(3 citation statements)
references
References 50 publications
0
3
0
Order By: Relevance
“…The idea of T-folds can be naturally extended to compactifications with S-duality twists (i.e. twisting by a symmetry of the equations of motion [105] ) or U-duality twists (U-folds) [6,7,106] and, given the understanding of mirror symmetry as T-duality [107], may allow mirror-folds for Calabi-Yau compactifications as first suggested in [6] (this concept has been studied in the context of K3 target spaces in [108,109,110]).…”
Section: T-foldsmentioning
confidence: 99%
“…The idea of T-folds can be naturally extended to compactifications with S-duality twists (i.e. twisting by a symmetry of the equations of motion [105] ) or U-duality twists (U-folds) [6,7,106] and, given the understanding of mirror symmetry as T-duality [107], may allow mirror-folds for Calabi-Yau compactifications as first suggested in [6] (this concept has been studied in the context of K3 target spaces in [108,109,110]).…”
Section: T-foldsmentioning
confidence: 99%
“…which easily follows from 2G = E + E t . Quantum mechanically, the boundary conditions (4.13) are introduced by inserting a "duality wall" (see for instance [39] and the supersymmetric case discussed in [40]). The T-duality wall can be thought of as the dimensional reduction of the T (U(1)) theory, 5 and in general, to incorporate the M twist into the action we have to decompose M in terms of the generators…”
Section: T-duality Twistmentioning
confidence: 99%
“…Orbifolding by T-duality offers a manageable class of non-geometric backgrounds that are more clearly understood from the viewpoint of orbifold constructions. More broadly speaking, the automorphism group can be non-perturbative when we twist boundary conditions by S-duality (see for example [12,13,14,15]) or more generally Uduality [16,17,18]. Understanding these stringy monodrofolds [19] is not only interesting in its own right, but they may also have some implications for string cosmology [20,21,22,23], string phenomenology [24,25,26] and modern duality-covariant frameworks of string theory such as the likes of 'Double Field Theory' (see for example [27]) and gauged supergravity theories [28,29,30].…”
Section: Introductionmentioning
confidence: 99%