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We study the strong coupling dynamics of the heterotic E_8 x E_8 string theory on the orbifolds T^6/Z_3 and C^3/Z_3 using the duality with the Horava-Witten M-theory picture. This leads us to a conjecture about the low energy description of…

High Energy Physics - Theory · Physics 2014-11-18 O. J. Ganor , J. Sonnenschein

We re-examine the question of heterotic - heterotic string duality in six dimensions and argue that the $E_8\times E_8$ heterotic string, compactified on $K3$ with equal instanton numbers in the two $E_8$'s, has a self-duality that inverts…

High Energy Physics - Theory · Physics 2010-04-07 M. J. Duff , R. Minasian , Edward Witten

We consider a theory with the gauge group $E_8$ assuming that the gauge symmetry breaking pattern is $E_8 \to E_7 \times U_1 \to E_6 \times U_1 \to SO_{10} \times U_1 \to SU_5 \times U_1 \to SU_3 \times SU_2 \times U_1$ and vacuum…

High Energy Physics - Phenomenology · Physics 2024-02-06 Konstantin Stepanyantz

The weakly coupled vacuum of $E_8\otimes E_8$ heterotic string theory remains an attractive scenario for phenomenolgy and cosmology. The particle spectrum is reviewed and the issues of gauge coupling unification, dilaton stabilization and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Mary K. Gaillard

We consider heterotic string compactifications to four dimensions when instantons shrink to zero size. If the standard model gauge group originates from the new gauge symmetry associated with the small instantons singularity, then the…

High Energy Physics - Theory · Physics 2009-09-29 Karim Benakli , Yaron Oz

Recent developments involving strongly coupled superstrings are discussed from a phenomenological point of view. In particular, strongly coupled $E_8\times E'_8$ is described as an appropriate long-wavelength limit of M-theory, and some…

High Energy Physics - Theory · Physics 2007-05-23 D. V. Nanopoulos

We analyze in detail the anomaly cancellation conditions for the strongly coupled $E_8 \times E_8$ heterotic string introduced by Horava and Witten and find new features compared to the ten-dimensional Green-Schwarz mechanism. We project…

High Energy Physics - Theory · Physics 2009-10-30 E. Dudas , J. Mourad

The gauge coupling unification is investigated at the classical level under the assumptions that the gauge symmetry breaking chain is $E_8\to E_7\times U_1 \to E_6\times U_1 \to SO_{10}\times U_1 \to SU_5 \times U_1 \to SU_3 \times SU_2…

High Energy Physics - Phenomenology · Physics 2023-07-17 Konstantin Stepanyantz

The weakly coupled vacuum of $E_8\otimes E_8$ heterotic string theory remains an attractive scenario for particle physics. The particle spectrum and the issue of dilaton stabilization are reviewed. A specific model for hidden sector…

High Energy Physics - Phenomenology · Physics 2015-06-25 Mary K. Gaillard

We study the two-point correlators of the currents of the $E_8$ global symmetry in the $N=(1,0)$ superconformal six-dimensional theory as well as in the 4D superconformal theories upon toroidal compactification. From the high-energy…

High Energy Physics - Theory · Physics 2009-10-30 Yeuk-Kwan E. Cheung , Ori J. Ganor , Morten Krogh

The weakly coupled vacuum of E_8 x E_8 heterotic string theory remains a promising candidate for the underlying theory of the Standard Model. The particle spectrum and the issue of dilaton stabilization are reviewed. Specific models for…

High Energy Physics - Phenomenology · Physics 2007-05-23 Mary K. Gaillard

We propose that the ten-dimensional $E_8\times E_8$ heterotic string is related to an eleven-dimensional theory on the orbifold ${\bf R}^{10}\times {\bf S}^1/{\bf Z}_2$ in the same way that the Type IIA string in ten dimensions is related…

High Energy Physics - Theory · Physics 2010-04-07 Petr Horava , Edward Witten

We show that three-dimensional N=8 $Sp(N)$ and $SO(2N+1)$ gauge theories flow to the same strong coupling fixed point. As a consequence, the corresponding orientifold two-planes in type IIA string theory are described at strong coupling and…

High Energy Physics - Theory · Physics 2010-02-03 Savdeep Sethi

In this paper, we present a systematic analysis of eleven-dimensional supergravity on a manifold with boundary, which is believed to be relevant to the strong coupling limit of the $E_8\times E_8$ heterotic string. Gauge and gravitational…

High Energy Physics - Theory · Physics 2010-04-07 Petr Horava , Edward Witten

In a certain strong coupling limit, compactification of the $E_8\times E_8$ heterotic string on a Calabi-Yau manifold $X$ can be described by an eleven-dimensional theory compactified on $X\times \S^1/\Z_2$. In this limit, the usual…

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

It is well-known that the SO(32) and $E_8\times E_8$ heterotic strings can be continuously connected to each other in nine dimensions. Since the strong-coupling duals of these theories are respectively the SO(32) Type I theory and M-theory…

High Energy Physics - Theory · Physics 2009-08-18 Julie D. Blum , Keith R. Dienes

Heterotic strings on $R^6 \times K3$ generically appear to undergo some interesting new phase transition at that value of the string coupling for which the one of the six-dimensional gauge field kinetic energies changes sign. An exception…

High Energy Physics - Theory · Physics 2009-10-07 M. J. Duff , H. Lu , C. N. Pope

Recent measurements of the values of gauge coupling constants as well as neutrino properties support the idea of a grand unified (GUT) description of particle physics at a large scale of $M_{GUT}\sim 10^{16}$ GeV. We discuss a strategy to…

High Energy Physics - Theory · Physics 2015-06-26 Hans Peter Nilles

Three-dimensional string theories with 16 supersymmetries are believed to possess a non-perturbative U-duality symmetry $SO(8,24,\Zint)$. By covariantizing the heterotic one-loop amplitude under U-duality, we propose an exact expression for…

High Energy Physics - Theory · Physics 2009-10-31 N. A. Obers , B. Pioline

We show the existence of global gauge anomalies in six dimensions for gauge groups SU(2),SU(3) and G_2 coupled to matter, characterized by an element of Z_{12},Z_6 and Z_3 respectively. Consideration of this anomaly rules out some of the…

High Energy Physics - Theory · Physics 2008-02-03 Michael Bershadsky , Cumrun Vafa
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