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We investigate the perturbative and non-perturbative correspondence of a class of four dimensional dual string constructions with N=4 and N=2 supersymmetry, obtained as Z_2 or Z_2 x Z_2 orbifolds of the type II, heterotic and type I string.…

High Energy Physics - Theory · Physics 2010-02-03 Andrea Gregori

In this article we review four-dimensional string vacua with N=2 space-time supersymmetry. In particular, we will discuss several aspects of the string-string duality between the heterotic string, compactified on $K3\times T^2$, and the…

High Energy Physics - Theory · Physics 2015-06-26 Dieter Lust

Null strings, strings with Carrollian worldsheets, are traditionally described by the Isberg-Lindstr\"om-Sundborg-Theodoridis (ILST) action, which is obtained via a tensionless limit of standard tensile strings. In a recent work, we…

High Energy Physics - Theory · Physics 2026-05-29 M. M. Sheikh-Jabbari , H. Yavartanoo

We report a physical origin of tensionless strings, obtained by formulating string dynamics in finite-lifetime settings for the first time. Departing from the conventional paradigm of eternal strings, we construct an inertial worldsheet…

High Energy Physics - Theory · Physics 2026-04-08 Sudip Karan , Bibhas Ranjan Majhi

Nonstandard parafermions are built and their central charges and dimensions are calculated. We then construct new N=2 superconformal field theories by tensoring the parafermions with a free boson. We study the spectrum and modular…

High Energy Physics - Theory · Physics 2015-05-28 Andrei Babichenko , Doron Gepner

A study is made of the implications of heterotic string $T$-duality and extended gauge symmetry for the conjectured equivalence of heterotic and Type I superstrings. While at first sight heterotic string world-sheet dynamics appears to…

High Energy Physics - Theory · Physics 2010-04-07 Joseph Polchinski , Edward Witten

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

A non-supersymmetric ten-dimensional open string theory is constructed as an orbifold of type I string theory, and as an orientifold of the bosonic type B theory. It is purely bosonic, and cancellation of massless tadpoles requires the…

High Energy Physics - Theory · Physics 2014-11-18 Oren Bergman , Matthias R. Gaberdiel

Recently, Kim, Shiu and Vafa proposed general consistency conditions for six dimensional supergravity theories with minimal supersymmetry coming from couplings to strings. We test them in explicit perturbative orientifold models in order to…

High Energy Physics - Theory · Physics 2020-12-30 Carlo Angelantonj , Quentin Bonnefoy , Cezar Condeescu , Emilian Dudas

We analyze topological string theory on a two dimensional torus, focusing on symmetries in the matter sector. Even before coupling to gravity, the topological torus has an infinite number of point-like physical observables, which give rise…

High Energy Physics - Theory · Physics 2009-10-22 Petr Horava

A $D>2$ topological string is presented by coupling the $2d$ topological gravity with the twisted version of the $N=2$ superconformal matter with $c=3k/(k-2)$. The latter is shown to admit $k+1$ chiral primary fields from the…

High Energy Physics - Theory · Physics 2008-02-03 Feng Yu

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

The 26 dimensional bosonic string, first suggested by Nambu and Goto, is reduced to a four dimensional superstring by using two species of 6 and 5 Majorana fermions as proposed by Deo. These two species of fermions differ in their…

High Energy Physics - Theory · Physics 2010-04-21 B. B. Deo , P. K. Jena

Is perturbative stability intimately tied with the existence of spacetime fermions in string theory in more than two dimensions? Type 0'B string theory in ten-dimensional flat space is a rare example of a non-tachyonic, non-supersymmetric…

High Energy Physics - Theory · Physics 2009-04-17 Dan Israel , Vasilis Niarchos

We construct D=4 Type I vacua with massless content remarkably close to that of the standard model of particle physics. They are tachyon-free non-supersymmetric models which are obtained starting with a standard D=4, N=1 compact Type IIB…

High Energy Physics - Theory · Physics 2014-11-18 G. Aldazabal , L. E. Ibanez , F. Quevedo

Over the past three decades, considerable effort has been devoted to studying the rich and diverse phenomenologies of heterotic strings exhibiting spacetime supersymmetry. Unfortunately, during this same period, there has been relatively…

High Energy Physics - Theory · Physics 2015-07-01 Steven Abel , Keith R. Dienes , Eirini Mavroudi

We construct a tensionless string model in a four-dimensional space-time ${\bf R}^{2,2}$ with the (2,2) signature and solve the string equations. We find that the signature change radically changes the structure of the holonomy group of the…

High Energy Physics - Theory · Physics 2007-05-23 S. A. Pol'shin , A. A. Zheltukhin

In recent work Kachru, Kumar and Silverstein introduced a special class of non-supersymmetric type II string theories in which the cosmological constant vanishes at the first two orders of perturbation theory. Heuristic arguments suggest…

High Energy Physics - Theory · Physics 2011-02-02 Jeffrey A. Harvey

We present an alternative $N=(4,0)$ superstring theory, with field content different from that of previously-known $N=(4,0)$ superstring theories. This theory is presented as a non-linear $\s$-model on the coset $SU(n,1) / SU(n) \otimes…

High Energy Physics - Theory · Physics 2009-10-28 Hitoshi Nishino

After introducing a d=10 pure spinor $\lambda^\alpha$, the Virasoro constraint $\partial x^m \partial x_m =0$ can be replaced by the twistor-like constraint $\partial x^m (\gamma_m \lambda)_\alpha=0$. Quantizing this twistor-like constraint…

High Energy Physics - Theory · Physics 2015-03-16 Nathan Berkovits