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Related papers: Point-like Instantons on K3 Orbifolds

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In this paper we study compactifications of the ${\cal N}=2$ heterotic $E_8\times E_8$ string on $(K3\times T^2)/\mathbb{Z}_3$ with various gauge backgrounds and calculate the topological couplings in the effective supergravity action that…

High Energy Physics - Theory · Physics 2020-05-20 Andreas Banlaki , Aradhita Chattopadhyaya , Abhiram Kidambi , Thorsten Schimannek , Maria Schimpf

We construct, as hypersurfaces in toric varieties, Calabi-Yau manifolds corresponding to F-theory vacua dual to E8*E8 heterotic strings compactified to six dimensions on K3 surfaces with non-semisimple gauge backgrounds. These vacua were…

High Energy Physics - Theory · Physics 2009-10-30 Philip Candelas , Eugene Perevalov , Govindan Rajesh

Effective field theories in type I and II superstring theories for D-branes located at points in the orbifold C^2/Z_n are supersymmetric gauge theories whose field content is conveniently summarized by a `quiver diagram,' and whose…

High Energy Physics - Theory · Physics 2008-02-03 Michael R. Douglas , Gregory Moore

A detailed understanding of instanton effects for half-BPS couplings is pursued in theories with 16 supersymmetries. In particular, we investigate the duality between heterotic string on $T^4$ and type IIA on $K_3$ at the $T^4/Z_2$ orbifold…

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

In this paper we consider the role that worldsheet instantons in the heterotic string could play in spin-statistics violations. Such violations are nonperturbative in the string tension and so would not appear in the spacetime effective…

High Energy Physics - Theory · Physics 2008-11-26 Mark G. Jackson

F-theory/heterotic duality is formulated in the stable degeneration limit of a K3 fibration on the F-theory side. In this note, we analyze the structure of the stable degeneration limit. We discuss whether stable degeneration exists for…

High Energy Physics - Theory · Physics 2018-03-13 Yusuke Kimura

According to a recent classification of 6d (1,0) theories within F-theory there are only six "pure" 6d gauge theories which have a UV superconformal fixed point. The corresponding gauge groups are $SU(3),SO(8),F_4,E_6,E_7$, and $E_8$. These…

High Energy Physics - Theory · Physics 2017-10-25 Michele Del Zotto , Guglielmo Lockhart

We study the deformation theory of $\mathrm{G}_2$-instantons on nearly $\mathrm{G}_2$ manifolds. There is a one-to-one correspondence between nearly parallel $\mathrm{G}_2$ structures and real Killing spinors, thus the deformation theory…

Differential Geometry · Mathematics 2022-08-30 Ragini Singhal

We construct new supersymmetric NS(-1)-branes supported by the $SU(2)\times SU(2)$ 't Hooft instantons in ${\cal N}=1$, $D=4$ supergravity. We show that although the magnetic 3-form string flux is invariant under the variation of instanton…

High Energy Physics - Theory · Physics 2025-07-09 Liang Ma , H. Lu

We derive a single field slow-roll inflaton potential in three intersecting $D7$ branes configuration under type IIB/F-theory compactification. Among three resulting K\"{a}hler moduli corresponding to three orthogonal directions, two are…

High Energy Physics - Theory · Physics 2023-05-08 Abhijit Let , Arunoday Sarkar , Chitrak Sarkar , Buddhadeb Ghosh

We compute the gravitational coupling $F_1$ for IIA string theory on $K3 \times T^2$ and use string-string duality to deduce the corresponding term for heterotic string on $T^6$. The latter is an infinite sum of gravitational instanton…

High Energy Physics - Theory · Physics 2016-08-25 Jeffrey A. Harvey , Gregory Moore

The (I)nstantonic strings are described as extended states occupying a flat (isometry) direction on the multiple M5-brane world-volume. These are constituted by 4-dimensional gauge instantons and 2-dimensional chiral axion. In this light we…

High Energy Physics - Theory · Physics 2017-04-26 Harvendra Singh

We analyze N=2 (perturbative and non-perturbative) corrections to the effective theory in type I orbifold models where a dual heterotic description is available. These corrections may play an important role in phenomenological scenarios.…

High Energy Physics - Theory · Physics 2008-11-26 P. G. Camara , E. Dudas

Orbifold compactification of heterotic E8 x E8 string theory is a source for promising grand unified model building. It can accommodate the successful aspects of grand unification while avoiding problems like doublet-triplet splitting in…

High Energy Physics - Theory · Physics 2008-11-26 Stefan Forste , Hans Peter Nilles , Patrick K. S. Vaudrevange , Akin Wingerter

We study compactifications of Type IIB string theory on a K3 \times T^2/Z_2 orientifold in the presence of RR and NS flux. We find the most general supersymmetry preserving, Poincare invariant, vacua in this model. All the complex structure…

High Energy Physics - Theory · Physics 2010-11-19 Prasanta K. Tripathy , Sandip P. Trivedi

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 explore the deformation theory of instantons on locally conformal (LC) $Spin(7)$ manifolds. These structures, characterized by a non-parallel fundamental 4-form $\Phi$ satisfying $d\Phi = \theta \wedge \Phi$, represent a significant, yet…

Differential Geometry · Mathematics 2025-11-13 Eyup Yalcinkaya

It is shown that the Type IIA superstring compactified on $K3$ has a smooth string soliton with the same zero mode structure as the heterotic string compactified on a four torus, thus providing new evidence for a conjectured exact duality…

High Energy Physics - Theory · Physics 2009-09-17 J. A. Harvey , A. Strominger

We study the global structure of vacua of heterotic strings compactified on orbifolds $T^4/Z_N$ (N=2,3) in the presence of heterotic 5-branes. Gauge symmetry breaking associated with orbifold is described by instantons in the field theory.…

High Energy Physics - Theory · Physics 2019-09-04 Kang-Sin Choi , Tatsuo Kobayashi

We analyze $M$-theory compactified on $(K3\times S^1)/Z_2$ where the $Z_2$ changes the sign of the three form gauge field, acts on $S^1$ as a parity transformation and on K3 as an involution with eight fixed points preserving SU(2)…

High Energy Physics - Theory · Physics 2009-09-15 Ashoke Sen
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