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We compute an SL(6,Z) invariant partition function for the chiral two-form of the M theory fivebrane compactified on the six-torus. From a manifestly SL(5,Z) invariant formalism, we prove that the partition function has an additional…

High Energy Physics - Theory · Physics 2010-11-15 Louise Dolan , Chiara R. Nappi

We study the partition function of type IIA string theory on 10-manifolds of the form T^2 x X where X is 8-dimensional, compact, and spin. We pay particular attention to the effects of the topological phases in the supergravity action…

High Energy Physics - Theory · Physics 2010-04-05 Gregory Moore , Natalia Saulina

We study the Type IIA NS five-brane wrapped on a Calabi-Yau manifold X in a double-scaled decoupling limit. We calculate the euclidean partition function in the presence of a flat RR 3-form field. The classical contribution is given by a…

High Energy Physics - Theory · Physics 2007-05-23 R. Dijkgraaf , E. Verlinde , M. Vonk

This paper continues the discussion of hep-th/0605038, applying the holographic formulation of self-dual theory to the Ramond-Ramond fields of type II supergravity. We formulate the RR partition function, in the presence of nontrivial…

High Energy Physics - Theory · Physics 2007-05-23 Dmitriy M. Belov , Gregory W. Moore

Computation of superstring partition function for the non-linear sigma model on the product of a two-torus and its dual within the scope of the doubled formalism is presented. We verify that it reproduces the partition functions of the…

High Energy Physics - Theory · Physics 2009-11-18 Sudipto Paul Chowdhury

On the world-volume of an $M$-theory five-brane propagates a two-form with self-dual field strength. As this field is non-Lagrangian, there is no obvious framework for determining its partition function. An analogous problem exists in Type…

High Energy Physics - Theory · Physics 2010-04-07 Edward Witten

We use holomorphic factorization to find the partition functions of an abelian two-form chiral gauge-field on a flat six-torus. We prove that exactly one of these partition functions is modular invariant. It turns out to be the one that…

High Energy Physics - Theory · Physics 2009-10-31 Andreas Gustavsson

The partition function of type IIA and B strings on R^6xK3, in the T^4/Z_2 orbifold limit, is explicitly computed as a modular invariant sum over spin strutures required by perturbative unitarity in order to extend the analysis to include…

High Energy Physics - Theory · Physics 2010-11-15 L. Dolan , M. Langham

We compute the partition function of four-dimensional abelian gauge theory on a general four-torus T4 with flat metric using Dirac quantization. In addition to an SL(4, Z) symmetry, it possesses SL(2,Z) symmetry that is electromagnetic…

High Energy Physics - Theory · Physics 2017-05-12 Louise Dolan , Yang Sun

Starting from the recent action proposed by Sen [1,2], we evaluate the partition function of the compact chiral boson on a two-dimensional torus using a path-integral formulation. Crucially, we use a Wick-rotation procedure obtained from a…

High Energy Physics - Theory · Physics 2022-05-11 Enrico Andriolo , Neil Lambert , Tristan Orchard , Constantinos Papageorgakis

We study the relation between class S theories on punctured tori and isomonodromic deformations of flat SL(N) connections on the two dimensional torus with punctures. Turning on the self dual $\Omega$-background corresponds to a…

High Energy Physics - Theory · Physics 2026-01-13 Giulio Bonelli , Fabrizio Del Monte , Pavlo Gavrylenko , Alessandro Tanzini

We compute the partition function of five-dimensional abelian gauge theory on a five-torus T5 with a general flat metric using the Dirac method of quantizing with constraints. We compare this with the partition function of a single…

High Energy Physics - Theory · Physics 2013-09-10 Louise Dolan , Yang Sun

We revisit partition functions of closed strings on toroidal backgrounds, including their $\mathbb{Z}_N$ shift orbifolds in the formalism where the dimension of the target space is doubled to make T-duality manifest. In such a T-duality…

High Energy Physics - Theory · Physics 2014-06-10 H. S. Tan

We present an attempt to formulate an action for the worldvolume theory of a single M5-brane, based on the splitting of the six worldvolume directions into 2+4, which breaks manifest Lorentz invariance from $SO(1,5)$ to $SO(1,1)\times…

High Energy Physics - Theory · Physics 2016-01-27 Sheng-Lan Ko , Pichet Vanichchapongjaroen

We evaluate quasi-classically the Ramond partition function of Euclidean D=10 U(N) super-Yang--Mills theory reduced to a two-dimensional torus. The result can be interpreted in terms of free strings wrapping the space-time torus, as…

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

Just as D-brane charge of Type IIA and Type IIB superstrings is classified, respectively, by K^1(X) and K(X), Ramond-Ramond fields in these theories are classified, respectively, by K(X) and K^1(X). By analyzing a recent proposal for how to…

High Energy Physics - Theory · Physics 2010-04-07 Gregory Moore , Edward Witten

Genus two partition functions of 2d chiral conformal field theories are given by Siegel modular forms. We compute their conformal blocks and use them to perform the conformal bootstrap. The advantage of this approach is that it imposes…

High Energy Physics - Theory · Physics 2017-05-18 Christoph A. Keller , Gregoire Mathys , Ida G. Zadeh

Superfield methods can be used to determine the precise way the self-dual five-form couples to the metric in the first non-trivial $\alpha'$ corrections to type IIB supergravity. We explicitly compute the exact tensor structure of these…

High Energy Physics - Theory · Physics 2010-04-22 M. F. Paulos

It has been shown recently that the toroidally compactified type IIB string effective action possesses an SL(2, R) invariance as a consequence of the corresponding symmetry in ten dimensions when the self-dual five-form field strength is…

High Energy Physics - Theory · Physics 2010-11-19 Shibaji Roy

A Siegel-type chiral p-form action is proposed in D=2(p+1) spacetime dimensions. The approach we adopt is to realize the symmetric second-rank Lagrange-multiplier field, introduced in Siegel's action, in terms of a normalized multiplication…

High Energy Physics - Theory · Physics 2009-11-07 Yan-Gang Miao , Harald J. W. Mueller-Kirsten , Dae Kil Park
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