ID: hep-th/9204040

On the Moduli Space of the $T^6/Z_3$ Orbifold and Its Modular Group

April 10, 1992

View on ArXiv
S. Ferrara, P. Frè, P. Soriani
High Energy Physics - Theory

We describe the duality group $\Gamma=SU(3,3,Z)$ for the Narain lattice of the $T^6/Z_3$ orbifold and its action on the corresponding moduli space. A symplectic embedding of the momenta and winding numbers allows us to connect the orbifold lattice to the special geometry of the moduli space. As an application, a formal expression for an automorphic function, which is a candidate for a non--perturbative superpotential, is given.

Similar papers 1

T-duality orbifolds of heterotic Narain compactifications

March 15, 2017

87% Match
Stefan Groot Nibbelink, Patrick K. S. Vaudrevange
High Energy Physics - Theory

To obtain a unified framework for symmetric and asymmetric heterotic orbifold constructions we provide a systematic study of Narain compactifications orbifolded by finite order T-duality subgroups. We review the generalized vielbein that parametrizes the Narain moduli space (i.e. the metric, the B-field and the Wilson lines) and introduce a convenient basis of generators of the heterotic T-duality group. Using this we generalize the space group description of orbifolds to Nar...

Find SimilarView on arXiv

SpaceTime Duality And $SU(n,1)\over SU(n)\otimes U(1)$ Cosets Of Orbifold Compactification

March 13, 1996

86% Match
W. A. Sabra
High Energy Physics - Theory

The duality symmetry group of the cosets ${\textstyle SU(n,1)\over \textstyle SU(n)\otimes U(1)}$, which describe the moduli space of a two-dimensional subspace of an orbifold model with $(n-1)$ complex Wilson lines moduli, is discussed. The full duality group and its explicit action on the moduli fields are derived.

Find SimilarView on arXiv

Anisotropic Solutions For Orbifold Moduli From Duality Invariant Gaugino Condensates

May 4, 1994

86% Match
D. Bailin, A. Love, ... , Thomas S.
High Energy Physics - Theory

The values of the $T$ and $U$ moduli are studied for those ${\bf Z}_N $ Coxeter orbifolds with the property that some of the twisted sectors have fixed planes for which the six-torus ${\bf T}^6 $ can not be decomposed into a direct sum ${\bf T}^2\bigoplus {\bf T}^4 $ with the fixed plane lying in ${\bf T}^2 $. Such moduli in general transform under a subgroup of the modular group $SL(2,Z).$ The moduli are determined by minimizing the effective potential derived from a duality...

Find SimilarView on arXiv

Duality Symmetries in Orbifold Models

September 24, 1993

85% Match
D. Bailin, A. Love, ... , Thomas S.
High Energy Physics - Theory

We derive the duality symmetries relevant to moduli dependent gauge coupling constant threshold corrections, in Coxeter $ {\bf Z_N} $ orbifolds. We consider those orbifolds for which the point group leaves fixed a 2-dimensional sublattice $\Lambda_2$, of the six dimensional torus lattice $\Lambda_6$, where $\Lambda_6 $ cannot be decomposed as $\Lambda_2 \bigoplus{\Lambda_4}.$

Find SimilarView on arXiv

Moduli Spaces and Target Space Duality Symmetries in $(0,2)\; Z_N$ Orbifold Theories with Continuous Wilson Lines

May 2, 1994

85% Match
G. Lopes Cardoso, D. Luest, T. Mohaupt
High Energy Physics - Theory

We present the coset structure of the untwisted moduli space of heterotic $(0,2) \; Z_N$ orbifold compactifications with continuous Wilson lines. For the cases where the internal 6-torus $T_6$ is given by the direct sum $T_4 \oplus T_2$, we explicitly construct the K\"{a}hler potentials associated with the underlying 2-torus $T_2$. We then discuss the transformation properties of these K\"{a}hler potentials under target space modular symmetries. For the case where the $Z_N$ t...

Find SimilarView on arXiv

Moduli Stabilization from Fluxes in a Simple IIB Orientifold

January 5, 2002

85% Match
Shamit Kachru, Michael Schulz, Sandip Trivedi
High Energy Physics - Theory

We study novel type IIB compactifications on the T^6/Z_2 orientifold. This geometry arises in the T-dual description of Type I theory on T^6, and one normally introduces 16 space-filling D3-branes to cancel the RR tadpoles. Here, we cancel the RR tadpoles either partially or fully by turning on three-form flux in the compact geometry. The resulting (super)potential for moduli is calculable. We demonstrate that one can find many examples of N=1 supersymmetric vacua with greatl...

Find SimilarView on arXiv

Classification and a toolbox for orientifold models

March 7, 2005

85% Match
P. Crete U, Ecole Polytechnique Anastasopoulos, A. B. Crete U, USTO Hammou
High Energy Physics - Theory

We provide the general tadpole conditions for a class of supersymmetric orientifold models by studing the general properties of the elements included in the orientifold group. In this talk, we concentrate on orientifold models of the type $T^6/Z_M\times Z_N$.

Find SimilarView on arXiv

The Quasicrystalline String Landscape

May 31, 2024

84% Match
Zihni Kaan Baykara, Houri-Christina Tarazi, Cumrun Vafa
High Energy Physics - Theory

In this work we investigate a largely unexplored non-geometric corner of the string landscape: the quasicrystalline orbifolds. These exist at special points of the Narain moduli leading to frozen moduli and large quantum symmetries. Here we complete the classification and construction of quasicrystalline Narain lattices and use this to explore supersymmetric compactifications in $4\leq D\leq 6$ and with $4\leq Q\leq 16$ supercharges, leading to novel theories including theori...

Find SimilarView on arXiv

Some comments on symmetric orbifolds of K3

February 28, 2019

84% Match
Roberto Volpato
High Energy Physics - Theory

We consider two dimensional $\mathcal{N}=(4,4)$ superconformal field theories in the moduli space of symmetric orbifolds of K3. We complete a classification of the discrete groups of symmetries of these models, conditional to a series of assumptions and with certain restrictions. Furthermore, we provide a partial classification of the set of twining genera, encoding the action of a discrete symmetry $g$ on a space of supersymmetric states in these models. These results sugges...

Find SimilarView on arXiv

Unifying the 6D $\mathcal{N}=(1,1)$ String Landscape

September 13, 2022

84% Match
Bernardo Fraiman, Freitas Héctor Parra De
High Energy Physics - Theory

We propose an organizing principle for string theory moduli spaces in six dimensions with $\mathcal{N} = (1,1)$, based on a rank reduction map, into which all known constructions fit. In the case of cyclic orbifolds, which are the main focus of the paper, we make an explicit connection with meromorphic 2D (s)CFTs with $c = 24$ ($c = 12$) and show how these encode every possible gauge symmetry enhancement in their associated 6D theories. These results generalize naturally to n...

Find SimilarView on arXiv