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Related papers: Topological Charge of ADHM Instanton on R^2_{NC}*R…

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We analytically calculate the topological charge of the noncommutative ADHM U(N) k-instanton using the Corrigan's identity and find that the result is exactly the instanton number k.

High Energy Physics - Theory · Physics 2009-11-07 Yu Tian , Chuan-Jie Zhu , Xing-Chang Song

We study in detail the ADHM construction of U(N) instantons on noncommutative Euclidean space-time R_{NC}^4 and noncommutative space R_{NC}^2 x R^2. We point out that the completeness condition in the ADHM construction could be invalidated…

High Energy Physics - Theory · Physics 2009-11-07 Chong-Sun Chu , Valentin V. Khoze , Gabriele Travaglini

We found an exact solution of elongated U(1) instanton on noncommutative R^4 for general instanton number k. The deformed ADHM equation was solved with general k and the gauge connection and the curvature were given explicitly. We also…

High Energy Physics - Theory · Physics 2010-02-03 Tomomi Ishikawa , Shin-Ichiro Kuroki , Akifumi Sako

We study U(1) and U(2) noncommutative instantons on R^2_{NC} x R^2_C based on the ADHM construction. It is shown that a mild singularity in the instanton solutions for both self-dual and anti-self-dual gauge fields always disappears in…

High Energy Physics - Theory · Physics 2009-11-07 Keun-Young Kim , Bum-Hoon Lee , Hyun Seok Yang

We study the U(1) and U(2) instanton solutions of gauge theory on general noncommutative $\bf{R}^4$. In all cases considered we obtain explicit results for the projection operators. In some cases we computed numerically the instanton charge…

High Energy Physics - Theory · Physics 2018-01-17 Yu Tian , Chuan-Jie Zhu

Non-singular instantons are shown to exist on noncommutative R^4 even with a U(1) gauge group. Their existence is primarily due to the noncommutativity of the space. The relation between U(1) instantons on noncommutative R^4 and the…

High Energy Physics - Theory · Physics 2008-11-26 Furuuchi Kazuyuki

We make some comments on noncommutative $U(N)$-instantons on $\mathbb{R}^4_{\theta}$. We elaborate on the equations for the ASD-connection for free modules. Further we make some remarks on the computation of the topological index of ADHM…

Differential Geometry · Mathematics 2015-03-06 Nikolay A. Ivanov

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

In noncommutative spaces, it is unknown whether the Pontrjagin class gives integer, as well as, the relation between the instanton number and Pontrjagin class is not clear. Here we define ``Instanton number'' by the size of $B_{\alpha}$ in…

High Energy Physics - Theory · Physics 2014-11-18 Tomomi Ishikawa , Shin-Ichiro Kuroki , Akifumi Sako

The basic objects of the ADHM construction are reformulated in terms of elements of the $A_{\theta}(R^4)$ algebra of the noncommutative $R_{\theta}^4$ space. This new formulation of the ADHM construction makes possible the explicit calculus…

High Energy Physics - Theory · Physics 2009-11-11 M. Lagraa

We give a \theta-deformed version of the ADHM construction of SU(2) instantons with arbitrary topological charge on the sphere S^4. Classically the instanton gauge fields are constructed from suitable monad data; we show that in the…

Quantum Algebra · Mathematics 2011-05-19 Simon Brain , Giovanni Landi

We study U(1) and U(2) instanton solutions on noncommutative R^4 based on the noncommutative version of ADHM equation proposed by Nekrasov and Schwarz. It is shown that the anti-self-dual gauge fields on self-dual noncommutative R^4…

High Energy Physics - Theory · Physics 2008-11-26 Keun-Young Kim , Bum-Hoon Lee , Hyun Seok Yang

We define a fixed point topological charge for the two-dimensional O(3) lattice sigma-model which is free of topological defects. We use this operator in combination with the fixed point action to measure the topological susceptibility for…

High Energy Physics - Lattice · Physics 2009-10-28 Marc Blatter , Rudolf Burkhalter , Peter Hasenfratz , Ferenc Niedermayer

We present a classification of SU(2) instantons on $T^2\times\mathbb{R}^2$ according to their asymptotic behaviour. We then study the existence of such instantons for different values of the asymptotic parameters, describing explicitly the…

Differential Geometry · Mathematics 2007-05-23 Marcos Jardim

An alternative method to the topological instanton solution for deriving an expression for the topological charge is presented. This alternative method involves the use of relativistic quantum field theory and covariant electrodynamics. In…

Mathematical Physics · Physics 2007-05-23 Joseph Saaty

We consider the low energy dynamics of charge two instantons on noncommutative $\mathbb{R}^{2}_{NC}\times\mathbb{R}^{2}_{NC}$ in U(2) 5-dimensional super-Yang-Mills, using the Manton approximation for slow-moving instantons to calculate the…

High Energy Physics - Theory · Physics 2015-05-19 Andrew Iskauskas , Douglas J. Smith

We discuss the Atiyah-Drinfeld-Hitchin-Manin (ADHM) construction of U(N) instantons in noncommutative (NC) space and prove the one-to-one correspondence between moduli spaces of the noncommutative instantons and the ADHM data, together with…

High Energy Physics - Theory · Physics 2013-11-22 Masashi Hamanaka , Toshio Nakatsu

We discuss instantons on noncommutative four-dimensional Euclidean space. In commutative case one can consider instantons directly on Euclidean space, then we should restrict ourselves to the gauge fields that are gauge equivalent to the…

High Energy Physics - Theory · Physics 2011-07-19 Albert Schwarz

We construct a five-parameter family of gauge-nonequivalent SU(2) instantons on a noncommutative four sphere $S_\theta^4$ and of topological charge equal to -1. These instantons are critical points of a gauge functional and satisfy…

Quantum Algebra · Mathematics 2008-11-26 Giovanni Landi , Walter D. van Suijlekom

We apply the ADHM instanton construction to SU(2) gauge theory on T^n x R^(4-n)for n=1,2,3,4. To do this we regard instantons on T^n x R^(4-n) as periodic (modulo gauge transformations) instantons on R^4. Since the R^4 topological charge of…

High Energy Physics - Theory · Physics 2009-10-31 C. Ford , J. M. Pawlowski , T. Tok , A. Wipf
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