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We study $U(N)$ SYM theories on spaces with orbifold singularities via an equivalent description in terms of gauge theories on smooth manifolds with insertions of Gukov-Witten and twist defects. The combined effect of the defects is to…

High Energy Physics - Theory · Physics 2026-05-26 Roman Mauch , Lorenzo Ruggeri

We deform the standard four dimensional $\N=1$ superspace by making the odd coordinates $\theta$ not anticommuting, but satisfying a Clifford algebra. Consistency determines the other commutation relations of the coordinates. In particular,…

High Energy Physics - Theory · Physics 2009-11-10 Nathan Seiberg

N=2 supersymmetric Yang--Mills theories coupled to matter are considered in the Wess--Zumino gauge. The supersymmetries are realized nonlinearly and the anticommutator between two susy charges gives, in addition to translations, gauge…

High Energy Physics - Theory · Physics 2010-11-01 Nicola Maggiore

We study three-dimensional supersymmetric quiver gauge theories with a non-simply laced global symmetry primarily focusing on framed affine $B_{N}$ quiver theories. Using a supersymmetric partition function on a three sphere, and its…

High Energy Physics - Theory · Physics 2017-09-20 Anindya Dey , Amihay Hanany , Peter Koroteev , Noppadol Mekareeya

We study the symmetries of the N=1 exactly marginal deformations of N=4 Super Yang-Mills theory. For generic values of the parameters, these deformations are known to break the SU(3) part of the R-symmetry group down to a discrete subgroup.…

High Energy Physics - Theory · Physics 2014-11-18 Teresia Mansson , Konstantinos Zoubos

Perturbative deformations of symmetry structures on noncommutative spaces are studied in view of noncommutative quantum field theories. The rigidity of enveloping algebras of semi-simple Lie algebras with respect to formal deformations is…

Quantum Algebra · Mathematics 2007-05-23 Christian Blohmann

Based on the construction by Hosomichi, Seong and Terashima we consider N=1 supersymmetric 5D Yang-Mills theory with matter on a five-sphere with radius r. This theory can be thought of as a deformation of the theory in flat space with…

High Energy Physics - Theory · Physics 2013-06-05 Johan Kallen , Jian Qiu , Maxim Zabzine

A matricial Darboux operator intertwining two one-dimensional stationary Dirac Hamiltonians is constructed. This operator is such that the potential of the second Dirac Hamiltonian as well as the corresponding eigenfunctions are determined…

Quantum Physics · Physics 2007-05-23 N. Debergh , A. A. Pecheritsin , B. F. Samsonov , B. Van den Bossche

We study generalized gauge theories engineered by taking the low energy limit of the $Dp$ branes wrapping $X \times T^{p-3}$, with $X$ a possibly singular surface in a Calabi-Yau fourfold $Z$. For toric $Z$ and $X$ the partition function…

High Energy Physics - Theory · Physics 2018-01-17 Nikita Nekrasov

On any space-like W-surface in the three-dimensional Minkowski space we introduce locally natural principal parameters and prove that such a surface is determined uniquely up to motion by a special invariant function, which satisfies a…

Differential Geometry · Mathematics 2014-11-14 Georgi Ganchev , Vesselka Mihova

Using holography, we study non-perturbative effects in M-theory on orientifolds from the analysis of the S^3 partition functions of dual field theories. We consider the S^3 partition functions of N=4 Yang-Mills theory with O(n) gauge…

High Energy Physics - Theory · Physics 2016-02-17 Kazumi Okuyama

We show that the vortex moduli space in non-abelian supersymmetric N=(2,2) gauge theories on the two dimensional plane with adjoint and anti-fundamental matter can be described as an holomorphic submanifold of the instanton moduli space in…

High Energy Physics - Theory · Physics 2015-05-27 Giulio Bonelli , Alessandro Tanzini , Jian Zhao

Nonlinearities in finite dimensions can be linearized by projecting them into infinite dimensions. Unfortunately, often the linear operator techniques that one would then use simply fail since the operators cannot be diagonalized. This…

Mathematical Physics · Physics 2016-08-09 Paul M. Riechers , James P. Crutchfield

We study $\mathcal{N}=2$ theories on four-dimensional manifolds that admit a Killing vector $v$ with isolated fixed points. It is possible to deform these theories by coupling position-dependent background fields to the flavor current…

High Energy Physics - Theory · Physics 2022-09-21 Usman Naseer , Charles Thull

We study N=1 super Liouville theory on worldsheets with and without boundary. Some basic correlation functions on a sphere or a disc are obtained using the properties of degenerate representations of superconformal algebra. Boundary states…

High Energy Physics - Theory · Physics 2008-11-26 Takeshi Fukuda , Kazuo Hosomichi

We compute the partition function on S^3 of 3d N=4 theories which arise as the low-energy limit of 4d N=4 super Yang-Mills theory on a segment or on a junction, and propose its 1d interpretation. We show that the partition function can be…

High Energy Physics - Theory · Physics 2011-08-16 Tatsuma Nishioka , Yuji Tachikawa , Masahito Yamazaki

We consider the extension of classical 2-dimensional topological quantum field theories to Klein topological quantum field theories which allow unorientable surfaces. We approach this using the theory of modular operads by introducing a new…

Geometric Topology · Mathematics 2013-06-03 Christopher Braun

We revisit the connection between relativistic orbital precession, the Laplace-Runge-Lenz symmetry, and the $t$-channel discontinuity of scattering amplitudes. Applying this to scalar-tensor theories of gravity, we compute the conservative…

High Energy Physics - Theory · Physics 2023-07-13 Anne-Christine Davis , Scott Melville

We study N = 4 quiver theories on the three-sphere. We compute partition functions using the localisation method by Kapustin et al. solving exactly the matrix integrals at finite N, as functions of mass and Fayet-Iliopoulos parameters. We…

High Energy Physics - Theory · Physics 2015-05-28 Sergio Benvenuti , Sara Pasquetti

Nekrasov's partition function is defined on a flat bundle of R^4 over S^1 called the Omega background. When the fibration is self-dual, the partition function is known to be equal to the topological string partition function, which computes…

High Energy Physics - Theory · Physics 2012-10-08 Yu Nakayama , Hirosi Ooguri