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Related papers: The heterotic prepotential from eleven dimensions

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We explore the moduli space of heterotic strings in two dimensions. In doing so, we introduce new lines of compactified theories with Spin(24) gauge symmetry and discuss compactifications with Wilson lines. The phase structure of d=2…

High Energy Physics - Theory · Physics 2008-11-26 Joshua L. Davis

We consider one of the simplest time-dependent backgrounds in M-theory, describing the shrinking away of the M-theory dimension with the other spatial dimensions static. As the M-theory dimension becomes small, the situation becomes…

High Energy Physics - Theory · Physics 2008-11-26 Gustavo Niz , Neil Turok

For compactifications of heterotic string theory, we elucidate simple cohomological conditions that lead to the vanishing of superpotential n-point couplings for all n. These results generalize some vanishing theorems for Yukawa couplings…

High Energy Physics - Theory · Physics 2024-06-28 James Gray

A compactification of the heterotic string is considered which describes a particle propagating in the symmetric space M = SO(9,1;Z)\SO(9,1;R)/SO(9;R) in interaction with excited states whose dynamics is (1+1)-dimensional. The model appears…

High Energy Physics - Theory · Physics 2009-10-30 Michael B. Green , David Kutasov

In this paper we study the reduction of heterotic string theory on SU(2)-structure backgrounds. We compute the bosonic low-energy gauged N=2 supergravity specified by the Killing vectors corresponding to the gauged isometries. We check that…

High Energy Physics - Theory · Physics 2009-10-29 Jan Louis , Danny Martinez-Pedrera , Andrei Micu

In these lectures, we review the main properties of the topological theory obtained by twisting the N=2 two-dimensional superconformal algebra, associated to supersymmetric string compactifications. In particular, we describe a set of…

High Energy Physics - Theory · Physics 2008-11-26 I. Antoniadis , S. Hohenegger

These lectures begin by reviewing the evidence for S duality of the toroidally compactified heterotic string in 4d that was obtained in the period 1992--94. Next they review recently discovered dualities that relate all five of the 10d…

High Energy Physics - Theory · Physics 2010-11-19 John H. Schwarz

The canonical analysis of Proca's theory in five dimensions with a compact dimension is performed. From the Proca five dimensional action, we perform the compactification process on a S^1/\mathbf{Z_2} orbifold, then, we analyze the four…

Mathematical Physics · Physics 2014-02-14 Alberto Escalante , Carlos L. Pando Lambruschini , Prihel Cavildo

We revisit the duality between heterotic string theory compactified on K3 x T^2 and type IIA compactified on a Calabi-Yau threefold X in the hypermultiplet sector. We derive an explicit map between the field variables of the respective…

High Energy Physics - Theory · Physics 2015-06-03 Jan Louis , Roberto Valandro

We present a complete solution of the constraints for three-dimensional N=2 conformal supergravity in terms of unconstrained prepotentials. This allows us to develop a prepotential description of the off-shell versions of N=2 Poincare and…

High Energy Physics - Theory · Physics 2015-06-11 Sergei M. Kuzenko

In this paper we discuss compactifications of M-theory to four dimensions on X \times S^1/Z_2, in which nonstandard embeddings in the E_8 \times E_8 vacuum gauge bundle are considered. At the level of the effective field theory description…

High Energy Physics - Phenomenology · Physics 2014-11-17 Zygmunt Lalak , Stefan Pokorski , Steven Thomas

In the framework of heterotic M-theory compactified on a Calabi-Yau threefold 'times' an interval, the relation between geometry and four-flux is derived {\it beyond first order}. Besides the case with general flux which cannot be described…

High Energy Physics - Theory · Physics 2014-11-18 Gottfried Curio , Axel Krause

We study soft SUSY breaking terms in heterotic M-theory. We show that both weakly and strongly coupled heterotic string models lead to the same relations of soft SUSY breaking terms, $A=-M$ and $m^2 = M^2/3$, up to $O((\alpha T/S)^2)$.

High Energy Physics - Phenomenology · Physics 2009-10-31 Tatsuo Kobayashi

We consider non perturbative effects in M-theory compactifications on a seven-manifold of G_2 holonomy arising from membranes wrapped on supersymmetric three-cycles. When membranes are wrapped on associative submanifolds they induce a…

High Energy Physics - Theory · Physics 2009-01-07 Rafael Hernandez

The M-theoretic Emergence Proposal claims that all of the terms in the low-energy action arise from quantum effects. After reviewing the current status of this proposal, we focus on four-dimensional compactifications with $N=2$…

High Energy Physics - Theory · Physics 2026-04-01 Manuel Artime , Ralph Blumenhagen , Aleksandar Gligovic , Panagiotis Leivadaros

The tree-level amplitude for the scattering of two gauge particles constrained to move on the two distinct boundaries of eleven-dimensional space-time in the Horava-Witten formulation of M-theory is constructed. At low momenta this…

High Energy Physics - Theory · Physics 2009-10-31 Tathagata Dasgupta , Matthias R. Gaberdiel , Michael B. Green

On compactification to six spacetime dimensions, the fundamental heterotic string admits as a soliton a dual string whose effective worldsheet action couples to the background fields of the dual formulation of six-dimensional supergravity.…

High Energy Physics - Theory · Physics 2010-11-01 M. J. Duff

We show the existence of a supersymmetry breaking mechanism in string theory, where N=4 supersymmetry is broken spontaneously to N=2 and N=1 with moduli dependent gravitino masses. The spectrum of the spontaneously broken theory with lower…

High Energy Physics - Theory · Physics 2009-10-30 E. Kiritsis , C. Kounnas

The strong coupling dynamics of string theories in dimension $d\geq 4$ are studied. It is argued, among other things, that eleven-dimensional supergravity arises as a low energy limit of the ten-dimensional Type IIA superstring, and that a…

High Energy Physics - Theory · Physics 2010-04-07 Edward Witten

We generalize recent methods regarding the construction of complete prepotentials of five dimensional SCFTs to two classes of rank-$N$ theories, i.e. the $X_{1,N}$ and the UV fixed point of the $SU(N+1)_0+2(N+1)$F gauge theories. Their…

High Energy Physics - Theory · Physics 2024-03-27 Francesco Mignosa