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Related papers: Small $E_8$ Instantons and Tensionless Non-critica…

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A free superstring with chiral N=2 supersymmetry in six dimensions is proposed. It couples to a two-form gauge field with a self-dual field strength. Compactification to four dimensions on a two-torus gives a strongly coupled N=4…

High Energy Physics - Theory · Physics 2007-05-23 John H. Schwarz

Bundles of strings which interact via short-ranged pair potentials are studied in two dimensions. The corresponding transfer matrix problem is solved analytically for arbitrary string number N by Bethe ansatz methods. Bundles consisting of…

Condensed Matter · Physics 2009-10-22 C. Hiergeist , M. Lassig , R. Lipowsky

We discuss heterotic string theories in two dimensions with gauge groups Spin(24) and Spin(8) x E_8. After compactification the theories exhibit a rich spectrum of states with both winding and momentum. At special points some of these…

High Energy Physics - Theory · Physics 2009-11-11 Joshua L. Davis , Finn Larsen , Nathan Seiberg

We review quantitative tests on the duality between the heterotic string on T^2 and F-theory on K3. On the heterotic side, certain threshold corrections to the effective action can be exactly computed at one-loop order, and the issue is to…

High Energy Physics - Theory · Physics 2007-05-23 W. Lerche

In this paper, we are going to put in a single consistent framework apparently unrelated pieces of information, i.e. zero-point length, extra-dimensions, string T-duality. More in details we are going to introduce a modified Kaluza-Klein…

General Relativity and Quantum Cosmology · Physics 2007-05-23 Euro Spallucci , Michele Fontanini

An intriguing class of 6d supersymmetric theories are known as little strings theories, which exhibit a rich network of T-dualities. A robust feature of these theories are their Higgs branches. Focusing on the little string theories that…

High Energy Physics - Theory · Physics 2023-12-21 Lorenzo Mansi , Marcus Sperling

We study the spacetime decay to nothing in string theory and M-theory. First we recall a nonsupersymmetric version of heterotic M-theory, in which bubbles of nothing -- connecting the two E_8 boundaries by a throat -- are expected to be…

High Energy Physics - Theory · Physics 2008-11-26 Petr Horava , Cynthia A. Keeler

We show that T-duality can be broken by nonperturbative effects in string coupling. The T-duality in question is that of the 2-torus when the heterotic string is compactified on K3 x T2. This case is compared carefully to a situation where…

High Energy Physics - Theory · Physics 2010-02-03 Paul S. Aspinwall , M. Ronen Plesser

The non-perturbative dynamics of quantum field theories is studied using theoretical tools inspired by string formalism. Two main lines are developed: the analysis of stringy instantons in a class of four-dimensional N=2 gauge theories and…

High Energy Physics - Theory · Physics 2012-10-23 Daniele Musso

We obtain the exact non-perturbative thresholds of $R^4$ terms in IIB string theory compactified to eight and seven dimensions. These thresholds are given by the perturbative tree-level and one-loop results together with the contribution of…

High Energy Physics - Theory · Physics 2010-04-06 Elias Kiritsis , Boris Pioline

One of the leading candidates for quantum gravity, viz. string theory, has the following features incorporated in it. (i) The full spacetime is higher dimensional, with (possibly) compact extra-dimensions; (ii) There is a natural minimal…

High Energy Physics - Theory · Physics 2014-11-18 Michele Fontanini , Euro Spallucci , T. Padmanabhan

The spatial string tension of a SU(N) gauge theory without quarks is calculated using gauge/string duality for 1.2T_c<T<3T_c. The result is remarkably consistent with the available lattice data for N=2,3. Some evidence is found that to…

High Energy Physics - Phenomenology · Physics 2008-11-26 Oleg Andreev

We describe cosmic F--term strings with exponentially small tension which are D3 branes wrapped on deformed $A_3$ singularities. We show that brane instanton effects which can be calculated after a geometric transition give rise to an…

High Energy Physics - Theory · Physics 2009-08-18 Edi Halyo

We show that there exist two 27 and one 27 bar of E6, net one D=4, N=1 chiral matter supermultiplet as zero modes localized on the intersection of two 5-branes in the E8 x E8 heterotic string theory. The smeared intersecting 5-brane…

High Energy Physics - Theory · Physics 2014-11-20 Tetsuji Kimura , Shun'ya Mizoguchi

We consider the tensor theory on coincident E8 5-branes compactified on a three torus. Using string theory, we predict that there must be distinct components in the moduli space of this theory.We argue that new superconformal field theories…

High Energy Physics - Theory · Physics 2014-11-18 Arjan Keurentjes , Savdeep Sethi

1. Preliminaries. 2. Heterotic string and motivations for large volume compactifications; 2.1 Gauge coupling unification; 2.2 Supersymmetry breaking by compactification. 3. M-theory on S^1/Z_2 \times Calabi-Yau. 4. Type I/I' string theory…

High Energy Physics - Theory · Physics 2007-05-23 I. Antoniadis

We give a simple proof of the known S-duality of Heterotic String theory compactified on a T^6. Using this S-duality we calculate the tensions for a class of BPS 5-branes in Heterotic String theory on a circle. One of these, the…

High Energy Physics - Theory · Physics 2010-02-03 Morten Krogh

We review the structure $D=6, N=1$ string vacua with emphasis on the different connections due to T-dualities and S-dualities. The topics discussed include: Anomaly cancellation; K3 and orbifold $D=6, N=1$ heterotic compactifications;…

High Energy Physics - Theory · Physics 2016-11-03 L. E. Ibanez , A. M. Uranga

A new class of twistor-like string models in four-dimensional space-time extended by the addition of six tensorial central charge (TCC) coordinates $z_{mn}$ is studied. The Hamiltonian of tensionless string in the extended space-time is…

High Energy Physics - Theory · Physics 2014-11-18 A. A. Zheltukhin , U. Lindström

A simple geometric description of T-duality is given by identifying the cotangent bundles of the original and the dual manifold. Strings propagate naturally in the cotangent bundle and the original and the dual string phase spaces are…

High Energy Physics - Theory · Physics 2009-10-28 C. Klimcik , P. Severa