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Related papers: Noncommutative instantons revisited

200 papers

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

Interpreting the coordinates of the quantum Euclidean space R_q^4 [the SO_q(4)-covariant noncommutative space] as the entries of a ``q-quaternion matrix'' we construct (anti)instanton solutions of a would-be q-deformed su(2) Yang-Mills…

High Energy Physics - Theory · Physics 2010-10-27 Gaetano Fiore

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

These are lecture notes for an introductory course on noncommutative field and gauge theory. We begin by reviewing quantum mechanics as the prototypical noncommutative theory, as well as the geometrical language of standard gauge theory.…

High Energy Physics - Theory · Physics 2023-10-02 Patrizia Vitale , Martina Adamo , Roukaya Dekhil , Diego Fernández-Silvestre

These notes aim at a pedagogical introduction to recent work on deformation of spaces and deformation of vector bundles over them, which are relevant both in mathematics and in physics, notably monopole and instanton bundles. We first…

Quantum Algebra · Mathematics 2009-11-11 Giovanni Landi

It is well-known that the charge of fermion is 0 or $\pm1$ in the U(1) gauge theory on noncommutative spacetime. Since the deviation from the standard model in particle physics has not yet observed, and so there may be no room to…

High Energy Physics - Theory · Physics 2007-05-23 Yoshitaka Okumura

We show that the moduli space of the $(2,0)$ and little-string theories compactified on $T^3$ with R-symmetry twists is equal to the moduli space of U(1) instantons on a non-commutative $T^4$. The moduli space of $U(q)$ instantons on a…

High Energy Physics - Theory · Physics 2007-05-23 Yeuk-Kwan E. Cheung , Ori J. Ganor , Morten Krogh , Andrei Yu. Mikhailov

Motivated by the recent construction of a translation-invariant renormalizable non-commutative model for a scalar field (see arXiv:0802.0791 [math-ph]), we introduce models for non-commutative U(1) gauge fields along the same lines. More…

High Energy Physics - Theory · Physics 2008-11-26 Daniel N. Blaschke , Francois Gieres , Erwin Kronberger , Manfred Schweda , Michael Wohlgenannt

$U(n\otimes m)\ast$ gauge field theory on noncommutative spacetime is formulated and the standard-like model with the symmetry ${\text{U}(3_c\otimes 2\otimes 1_{\text{\scriptsize$Y$}})\ast}$ is reconstructed based on it. $\text{U}(n+m)\ast$…

High Energy Physics - Theory · Physics 2007-05-23 Yoshitaka Okumura

We propose a constraint on the noncommutative gauge theory with U(N) gauge group which gives rise to a noncommutative version of the SU(N) gauge group. The baryon operator is also constructed.

High Energy Physics - Theory · Physics 2009-11-07 Chong-Sun Chu , Harald Dorn

We find classically stable solitons (instantons) in odd (even) dimensional scalar noncommutative field theories whose scalar potential, $V(\ph)$, has at least two minima. These solutions are bubbles of the false vacuum whose size is set by…

High Energy Physics - Theory · Physics 2009-10-31 Rajesh Gopakumar , Shiraz Minwalla , Andrew Strominger

We consider Ward's generalized self-duality equations for U(2r) Yang-Mills theory on R^{4k} and their Moyal deformation under self-dual noncommutativity. Employing an extended ADHM construction we find two kinds of explicit solutions, which…

High Energy Physics - Theory · Physics 2010-04-05 Tatiana A. Ivanova , Olaf Lechtenfeld

In this thesis noncommutative gauge theory is extended beyond the canonical case, i.e. to structures where the commutator no longer is a constant. In the first part noncommutative spaces created by star-products are studied. We are able to…

High Energy Physics - Theory · Physics 2007-05-23 Wolfgang Behr

Noncommutative U(1) gauge theory in 4-dimensions is shown to be equivalent in some scaling limit to an ordinary non-linear sigma model in 2-dimensions . The model in this regime is solvable and the corresponding exact beta function is…

High Energy Physics - Theory · Physics 2009-11-10 Badis Ydri

We consider pure SU(N) gauge theories defined on an orbifold lattice, analogous to the S^1/Z_2 gauge theory orbifolds of the continuum, which according to the perturbative analysis do not have a Higgs phase. Non-perturbatively the…

High Energy Physics - Lattice · Physics 2015-06-18 Nikos Irges , Francesco Knechtli

We construct (anti)instanton solutions of a would-be q-deformed su(2) Yang-Mills theory on the quantum Euclidean space R_q^4 [the SO_q(4)-covariant noncommutative space] by reinterpreting the function algebra on the latter as a q-quaternion…

High Energy Physics - Theory · Physics 2009-11-11 Gaetano Fiore

We present a pedagogical introduction into noncommutative gauge theories, their stringy origin, and non-perturbative effects, including monopole and instanton solutions

High Energy Physics - Theory · Physics 2017-08-23 Nikita A. Nekrasov

We establish the ultra-violet finiteness of various classes of noncommutative gauge theories.

High Energy Physics - Theory · Physics 2009-11-07 I. Jack , D. R. T. Jones

IR divergences of a non-commutative U(1) Maxwell theory are discussed at the one-loop level using an interpolating gauge to show that quadratic IR divergences are independent not only from a covariant gauge fixing but also independent from…

High Energy Physics - Theory · Physics 2009-11-11 M. Attems , D. N. Blaschke , M. Ortner , M. Schweda , S. Stricker , M. Weiretmayr

We extend the instanton calculus for N=1/2 U(2) supersymmetric gauge theory by including one massless flavor. We write the equations of motion at leading order in the coupling constant and we solve them exactly in the non(anti)commutativity…

High Energy Physics - Theory · Physics 2009-11-11 Simone Giombi , Riccardo Ricci , Daniel Robles-Llana , Diego Trancanelli