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We consider non-perturbative terms in the 4d effective action due to BPS D-brane instantons, and study their continuity properties in moduli space as instantons cross lines of BPS stability, potentially becoming non-BPS. We argue that BPS…

High Energy Physics - Theory · Physics 2009-10-09 Inaki Garcia-Etxebarria , Fernando Marchesano , Angel M. Uranga

We study the compatibility between the $BPST SU(2)$ instanton and the fuzzy four-sphere algebra. By using the projective module point of view as an intermediate step, we are able to identify a non-commutative solution of the matrix model…

High Energy Physics - Theory · Physics 2009-11-11 P. Valtancoli

We discuss the 't Hoof ansatz for instanton solutions in noncommutative U(2) Yang-Mills theory. We show that the extension of the ansatz leading to singular solutions in the commutative case, yields to non self-dual (or self-antidual)…

High Energy Physics - Theory · Physics 2009-11-07 D. H. Correa , G. S. Lozano , E. F. Moreno , F. A. Schaposnik

I review in this talk different approaches to the construction of vortex and instanton solutions in noncommutative field theories.

High Energy Physics - Theory · Physics 2017-08-23 Fidel A. Schaposnik

We study the instanton calculus for N=4 super Yang-Mills theory in ten-dimensional Omega-background with the R-symmetry Wilson line gauge field. From the ADHM construction of instantons in the background, we obtain the deformed instanton…

High Energy Physics - Theory · Physics 2015-06-03 Katsushi Ito , Hiroaki Nakajima , Takuya Saka , Shin Sasaki

We construct U(2) noncommutative multi-instanton solutions by extending Witten's ansatz [1] which reduces the problem of cylindrical symmetry in four dimensions to that of a set of Bogomol'nyi equations for an Abelian Higgsmodel in two…

High Energy Physics - Theory · Physics 2015-06-26 D. H. Correa , E. F. Moreno , F. A. Schaposnik

We present closed-form expressions of unrefined instanton partition functions for gauge groups of type $BCD$ as sums over Young diagrams. For $\mathrm{SO}(n)$ gauge groups, we provide a fivebrane web picture of our formula based on the…

High Energy Physics - Theory · Physics 2023-02-01 Satoshi Nawata , Rui-Dong Zhu

The ADHM constraints which implicitly specify instanton gauge field configurations are solved for the explicit general form of instantons with topological charge two and gauge group U(N).

High Energy Physics - Theory · Physics 2010-04-05 N. B. Pomeroy

We study chiral gauge-invariant operators on moduli spaces of G instantons for any classical group G on A-type ALE spaces using Hilbert Series (HS). Moduli spaces of instantons on an ALE space can be realized as Higgs branches of certain…

High Energy Physics - Theory · Physics 2014-02-10 Anindya Dey , Amihay Hanany , Noppadol Mekareeya , Diego Rodriguez-Gomez , Rak-Kyeong Seong

Fermion propagator of the Schwinger Model is revisited from the point of view of its infrared behavior. The values of anomalous dimensions are found in arbitrary covariant gauge and in all contributing instanton sectors. In the case of a…

High Energy Physics - Theory · Physics 2008-11-26 Tomasz Radozycki

A recently proposed correspondence between 4-dimensional N=2 SUSY SU(k) gauge theories on R^4/Z_m and SU(k) Toda-like theories with Z_m parafermionic symmetry is used to construct four-point N=1 super Liouville conformal block, which…

High Energy Physics - Theory · Physics 2011-10-03 A. Belavin , V. Belavin , M. Bershtein

We study a class of torsion-free sheaves on complex projective spaces which generalize the much studied mathematical instanton bundles. Instanton sheaves can be obtained as cohomologies of linear monads and are shown to be semistable if its…

Algebraic Geometry · Mathematics 2007-11-12 Marcos Jardim

The ADHM construction is a very strong scheme to construct the instantons in four dimensions. We study an ADHM construction of instantons in $4n~(n\geq2)$ dimensions by generalizing this scheme. The higher-dimensional ADHM construction…

High Energy Physics - Theory · Physics 2017-07-27 Koki Takesue

Following the construction of the projection operators on $T^2$ presented by Gopakumar, Headrick and Spradlin, we construct a set of projection operators on the integral noncommutative orbifold $T^2/G (G=Z_N, N=2, 3, 4, 6)$ which correspond…

High Energy Physics - Theory · Physics 2009-06-11 Hou Bo-yu , Shi Kangjie , Yang Zhan-ying

Given a fiber bundle $Z \to M \to B$ and a flat vector bundle $E \to M$ with a compatible action of a discrete group $G$, and regarding $B / G$ as the non-commutative space corresponding to the crossed product algebra, we construct an…

Differential Geometry · Mathematics 2017-01-19 Bing Kwan So , GuangXiang Su

A novel geometric model of a noncommutative plane has been constructed. We demonstrate that it can be construed as a toy model for describing and explaining the basic features of physics in a noncommutative spacetime from a field theory…

High Energy Physics - Theory · Physics 2009-11-10 Subir Ghosh

By exploiting the relation between static zero modes of massless Dirac operator and Kustaanheimo-Stiefel (Hopf) bundle sections, a general zero modes Ansatz which depends on an arbitrary real vector-function on $R^3$ is constructed.

High Energy Physics - Theory · Physics 2007-05-23 D. V. Aleynikov , E. A. Tolkachev

We investigate unitarily inequivalent representations of the algebra of operators in quantum field theory in the cases where there is a Fock representation of the commutation relations. We examine more closely the operational definition of…

High Energy Physics - Theory · Physics 2025-05-15 F. Sobrero , M. S. Soares , T. Guerreiro , N. F. Svaiter

Two main problems face the construction of noncommutative actions for gravity with star products: the complex metric and finding an invariant measure. The only gauge groups that could be used with star products are the unitary groups. I…

High Energy Physics - Theory · Physics 2015-06-26 A. H. Chamseddine

We revisit the well-studied D0-D4 system of D-branes and its relationship to the ADHM construction. It is well known that the D0-branes appear as instantons in the D4-brane worldvolume. We add a Wilson line to the D4-brane in the guise of…

High Energy Physics - Theory · Physics 2015-06-23 David Tong , Kenny Wong
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