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Related papers: Elliptic Genus of E-strings

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We study the elliptic genera of 6d strings based on their modular properties. They are weak Jacobi forms of weight 0, whose indices are determined from the 2d chiral anomalies. We propose the ansatz for the elliptic genera which reflects…

High Energy Physics - Theory · Physics 2018-10-23 Joonho Kim , Kimyeong Lee , Jaemo Park

We extend the analysis of arXiv:2208.11703 to the 6d $(1,0)$ SCFTs known as massive E-string theories, which can be engineered in massive Type IIA with $8-n_0<8$ D8-branes close to an O8$^-$ (or O8$^*$ if $n_0=8,9$). For each choice of…

High Energy Physics - Theory · Physics 2023-03-16 Marco Fazzi , Simone Giacomelli , Suvendu Giri

A number of N=2 gauge theories can be realized by brane configurations in Type IIA string theory. One way of solving them involves lifting the brane configuration to M-theory. In this paper we present an alternative way of analyzing a…

High Energy Physics - Theory · Physics 2009-10-31 Anton Kapustin

We examine the conjecture that an 11d E_8 bundle, appearing in the calculation of phases in the M-Theory partition function, plays a physical role in M-Theory, focusing on consequences for the classification of string theory solitons. This…

High Energy Physics - Theory · Physics 2011-02-18 Allan Adams , Jarah Evslin

In this note we investigate certain topological aspects of the effective action of the NS5-brane in type IIA string theory. To facilitate the study of the corresponding partition function, we define a cohomology class whose vanishing is a…

High Energy Physics - Theory · Physics 2014-11-04 Hisham Sati

Two different mechanisms exist in non-perturbative String / M- theory for enhanced SU(N) (SO(2N)) gauge symmetries. It can appear in type IIA string theory or M-theory near an $A_{N-1}$ (D_N) type singularity where membrnes wrapped around…

High Energy Physics - Theory · Physics 2010-02-04 Ashoke Sen

We present brane constructions in Type IIA string theory for N=1 supersymmetric SO and Sp gauge theories with tensor representations using an orientifold 6-plane. One limit of these set-ups corresponds to N=2 theories previously constructed…

High Energy Physics - Theory · Physics 2009-09-17 Csaba Csaki , Martin Schmaltz , Witold Skiba , John Terning

In an earlier work it was shown that the IR singularities arising in the nonplanar one loop two point function of a noncommutative ${\cal N}=2$ gauge theory can be reproduced exactly from the massless closed string exchanges. The…

High Energy Physics - Theory · Physics 2009-11-11 Swarnendu Sarkar

In this talk we give a brief review of the algebraic structure behind the open and closed topological strings and $D$-branes and emphasize the role of tensor category and the Frobenius algebra. Also, we speculate on the possibility of…

High Energy Physics - Theory · Physics 2007-05-23 Ion V. Vancea

We compute the elliptic genera of two-dimensional N=(2,2) and N=(0,2) gauged linear sigma models via supersymmetric localization, for rank-one gauge groups. The elliptic genus is expressed as a sum over residues of a meromorphic function…

High Energy Physics - Theory · Physics 2014-03-18 Francesco Benini , Richard Eager , Kentaro Hori , Yuji Tachikawa

We construct a class of supersymmetric vacua of type IIB string theory describing systems of three- and seven-branes non-perturbatively completed by brane instantons. The vacua are specified by a set of holomorphic functions defined over a…

High Energy Physics - Theory · Physics 2015-06-05 Luca Martucci , Jose F. Morales , Daniel Ricci Pacifici

It is an old speculation that SU(N) gauge theory can alternatively be formulated as a string theory. Recently this subject has been revived, in the wake of the discovery of D-branes. In particular, it has been argued that at least some…

High Energy Physics - Lattice · Physics 2016-12-28 Christof Schmidhuber

We study string theory propagating on R^6 times K3 by constructing orientifolds of Type IIB string theory compactified on the T^4/Z_N orbifold limits of the K3 surface. This generalises the Z_2 case studied previously. The orientifold…

High Energy Physics - Theory · Physics 2014-11-18 Eric G. Gimon , Clifford V. Johnson

We improve on a recently constructed graphical representation of the supergravity 7-brane solution and apply this refined representation to re-study the open string description of the A-D-E-singularities in F-theory on K3. A noteworthy…

High Energy Physics - Theory · Physics 2010-02-11 Eric A. Bergshoeff , Jelle Hartong

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

Based on the recently discovered K-theory description of D-branes in string theory a K-theory interpretation of the topology of gauge conditions for four dimensional gauge theories, in particular 't Hooft abelian projection, is presented.…

High Energy Physics - Theory · Physics 2009-11-07 Cesar Gomez

We study the stringy instanton partition function of four dimensional ${\cal N}=2$ $U(N)$ supersymmetric gauge theory which was obtained by Bonelli et al in 2013. In type IIB string theory on $\mathbb{C}^2\times T^*\mathbb{P}^1\times…

High Energy Physics - Theory · Physics 2015-07-21 Masahide Manabe

6-dimensional superconformal field theories are exotic and fascinating. They emerge from compactifications of F-theory on Calabi-Yau elliptic fibrations, which grants them a rich array of dualities with various other formulations of string…

High Energy Physics - Theory · Physics 2024-02-12 David Jaramillo Duque

We study partition function of four-dimensional $\mathcal{N}=1$ supersymmetric field theory on $T^2 \times S^2$. By applying supersymmetry localization, we show that the $T^2 \times S^2$ partition function is given by elliptic genus of…

High Energy Physics - Theory · Physics 2015-04-17 Masazumi Honda , Yutaka Yoshida

The topological part of the M-theory partition function was shown by Witten to be encoded in the index of an E8 bundle in eleven dimensions. This partition function is, however, not automatically anomaly-free. We observe here that the…

High Energy Physics - Theory · Physics 2007-05-23 Igor Kriz , Hisham Sati