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Related papers: A Matrix Model for Heterotic $Spin(32)/Z_2$ and Ty…

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We develop a matrix model for the SO(32) Heterotic string with certain Wilson lines on the lightlike circle. This is done by using appropriate T-dualities. The method works for an infinite number of Wilson lines, but not for all. The matrix…

High Energy Physics - Theory · Physics 2009-10-31 Morten Krogh

We propose a nonperturbative framework for the O(32) type I open and closed string theory. The short distance degrees of freedom are bosonic and fermionic hermitian matrices belonging respectively to the adjoint and fundamental…

High Energy Physics - Theory · Physics 2012-01-25 Shyamoli Chaudhuri

We give a complete classification of Z_N orbifold compactification of the heterotic SO(32) string theory and show its potential for realistic model building. The appearance of spinor representations of SO(2n) groups is analyzed in detail.…

High Energy Physics - Theory · Physics 2010-02-03 Hans Peter Nilles , Saul Ramos-Sanchez , Patrick K. S. Vaudrevange , Akin Wingerter

The finite N version of Matrix theory describes M-theory and superstrings in so-called discretized light cone quantization (DLCQ). Its role has been explained for M-theory in 11 dimensions and for type IIA theory. We show novelties which…

High Energy Physics - Theory · Physics 2008-02-03 Lubos Motl , Leonard Susskind

We review here some of the checks of string-string duality between N=2, D=4 Heterotic and Type II models. The heterotic low energy field theory is reproduced on the type II side. It is also shown to be a generalization in the string context…

High Energy Physics - Theory · Physics 2009-10-30 H. Partouche

M-theory suggests the large N limit of the matrix description of a collection of N Type IA D-particles should provide a nonperturbative formulation of heterotic string theory. In this paper states in the matrix theory corresponding to…

High Energy Physics - Theory · Physics 2009-10-30 David A. Lowe

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

Following recent proposal of Dijkgraaf, Verlinde and Verlinde, we show that the M(atrix) theory compactified on $S_1/Z_2$ provides with a non-perturbative description of second-quantized light-cone heterotic string. This so-called heterotic…

High Energy Physics - Theory · Physics 2016-09-06 Soo-Jong Rey

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 propose that type 0B string theory in two dimensions admits a dual description in terms of a one dimensional bosonic matrix model of a hermitian matrix. The potential in the matrix model is symmetric with respect to the parity-like Z_2…

High Energy Physics - Theory · Physics 2016-09-06 Tadashi Takayanagi , Nicolaos Toumbas

We study a $U(N)$-invariant vector+matrix chain with the color structure of a lattice gauge theory with quarks and interpret it as a theory of open andclosed strings with target space $\Z$. The string field theory is constructed as a…

High Energy Physics - Theory · Physics 2014-11-18 Ivan K. Kostov

Characters of $E_8\otimes E_8$ and SO(32) heterotic strings involving the full internal symmetry Cartan subalgebra generators are defined after circle compactification so that they are T dual. The novel point, as compared with an earlier…

High Energy Physics - Theory · Physics 2009-10-31 Jean-Loup Gervais

We study the R -> 0 limit for heterotic strings of either kind (Spin(32)/Z_2 or E_8 x E_8) compactified on a circle, in the presence of an arbitrary Wilson line. Though for generic Wilson line this limit leads to chaotic behaviour, there…

High Energy Physics - Theory · Physics 2007-05-23 Arjan Keurentjes

Cobordism offers a unique perspective into the non-perturbative sector of string theory by demanding the absence of higher form global symmetries for quantum gravitational consistency. In this work we compute the spin cobordism groups of…

High Energy Physics - Theory · Physics 2024-09-19 Christian Kneissl

It is shown that the heterotic string emerges as a soliton in the type I superstring theory in ten dimensions. The collective coordinates of the soliton are described by a smooth, chiral worldsheet theory. There are eight bosonic and eight…

High Energy Physics - Theory · Physics 2009-10-28 Atish Dabholkar

The BPS spectrum of type I' string theory in a generic background is derived using the duality with the nine-dimensional heterotic string theory with Wilson lines. It is shown that the corresponding mass formula has a natural interpretation…

High Energy Physics - Theory · Physics 2009-10-30 O. Bergman , M. R. Gaberdiel , G. Lifschytz

The SO(32) theory, in the limit where it is an open superstring theory, is completely specified in the light-cone gauge as a second-quantized string theory in terms of a ``matrix string'' model. The theory is defined by the neighbourhood of…

High Energy Physics - Theory · Physics 2009-10-31 Clifford V. Johnson

We study modular symmetries in non-supersymmetric heterotic string theories on toroidal backgrounds with Wilson line modulus, constructed by stringy Scherk-Schwartz compactification. In particular, we focus on a subgroup of the T-duality…

High Energy Physics - Theory · Physics 2025-04-03 Shuta Funakoshi , Yuichi Koga , Hajime Otsuka

We study the Levin-Wen string-net model with a $Z_N$ type fusion algebra. Solutions of the local constraints of this model correspond to $Z_N$ gauge theory and double Chern-simons theories with quantum groups. For the first time, we…

Other Condensed Matter · Physics 2012-12-21 Ling-Yan Hung , Yidun Wan

Four dimensional heterotic SO(32) orbifold models are classified systematically with model building applications in mind. We obtain all Z3, Z7 and Z2N models based on vectorial gauge shifts. The resulting gauge groups are reminiscent of…

High Energy Physics - Theory · Physics 2010-02-03 Kang-Sin Choi , Stefan Groot Nibbelink , Michele Trapletti
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