Abstract

A rich pattern of gauge symmetries is found in the moduli space of heterotic string toroidal compactifications, at fixed points of the T-duality transformations. We analyze this pattern for generic tori, and scrutinize in full detail compactifications on a circle, where we find all the maximal gauge symmetry groups and the points where they arise. We present figures of two-dimensional slices of the 17-dimensional moduli space of Wilson lines and circle radii, showing the rich pattern of points and curves of symmetry enhancement. We then study the target space realization of the duality symmetry. Although the global continuous duality symmetries of dimensionally reduced heterotic supergravity are completely broken by the structure constants of the maximally enhanced gauge groups, the low energy effective action can be written in a manifestly duality covariant form using heterotic double field theory. As a byproduct, we show that a unique deformation of the generalized diffeomorphisms accounts for both SO(32) and E8 × E8 heterotic effective field theories, which can thus be considered two different backgrounds of the same double field theory even before compactification. Finally we discuss the spontaneous gauge symmetry breaking and Higgs mechanism that occurs when slightly perturbing the background fields, both from the string and the field theory perspectives.

Highlights

  • The distinct backgrounds of heterotic string theory on a k dimensional torus with constant metric, antisymmetric tensor field and Wilson lines are characterized by the points of theO(k,k+16;R) O(k;R)×O(k+16;R)×O(k,k+16;Z)coset manifold, where O(k, k + 16; Z) is theT-duality group [1, 2]

  • Comparing the string theory results with the spontaneous gauge symmetry breaking and Higgs mechanism in double field theory (DFT), we see that the masses acquired by the sligthly massive string states fully agree with those of the DFT fields, provided there is a specific relation between the vacuum expectation value of the scalars along the Cartan directions of the gauge group and the deviation of the metric, B-field and Wilson lines from the point of enhancement

  • In this paper we have analysed compactifications of the heterotic string on T k, focusing on the phenomenon of symmetry enhancement arising at special points and curves in moduli space

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Summary

Introduction

The distinct backgrounds of heterotic string theory on a k dimensional torus with constant metric, antisymmetric tensor field and Wilson lines are characterized by the points of the. The global duality symmetries are not manifest in heterotic supergravity To manifestly display these symmetries, as well as to account for the maximally enhanced gauge groups in a field theoretical setting, one appeals to the double field theory/generalized geometric reformulation of the string effective actions [9,10,11,12,13,14,15,16] (for reviews and more references see [17,18,19,20,21]). Comparing the string theory results with the spontaneous gauge symmetry breaking and Higgs mechanism in DFT, we see that the masses acquired by the sligthly massive string states fully agree with those of the DFT fields, provided there is a specific relation between the vacuum expectation value of the scalars along the Cartan directions of the gauge group and the deviation of the metric, B-field and Wilson lines from the point of enhancement. We count the number of non-vanishing structure constants of SO(32) and E8 × E8 in appendix G

Compactifications on T k
R sector
Massless spectrum
Compactifications on a circle
Enhancement-breaking of gauge symmetry
Exploring a slice of moduli space
T-duality in circle compactifications
More general dualities and fixed points
Effective action and Higgs mechanism
Effective action of massless states
Higgs mechanism in string theory
Heterotic double field theory
Gauged double field theory
Parameterization and choice of section
Generalized Scherk-Schwarz reductions
Fluctuations around generic points in moduli space
Symmetry enhancement
Away from the self-dual points
Comparison with string theory
Summary and outlook
A Lie algebras and lattices
That is
A21 2 R2
Full Text
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