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There are $N-1$ classes of kink solutions in $SU(N)\times Z_2$. We show how interactions between various kinks depend on the classes of individual kinks as well as on their orientations with respect to each other in the internal space. In…

High Energy Physics - Theory · Physics 2009-11-07 Levon Pogosian

We compute the one-loop quark-photon vertex and the quark magnetic moment in three different models with an infrared-modified gluon propagator, namely: the massive (Curci-Ferrari-like) model, the Gribov-Zwanziger model, and the Refined…

High Energy Physics - Phenomenology · Physics 2023-11-27 C. Mena , L. F. Palhares

In the two-dimensional CP(N-1) model one can parametrize exact many-instanton solutions via N `constituents' (called `zindons'). This parameterization allows, in principle, a complete `melting' of individual instantons. The model is…

High Energy Physics - Lattice · Physics 2017-08-23 M. Maul , D. Diakonov

The multi-instanton solutions by 'tHooft and Jackiw, Nohl & Rebbi are generalized to curvilinear coordinates. Expressions can be notably simplified by the appropriate gauge transformation. This generates the compensating addition to the…

High Energy Physics - Theory · Physics 2009-10-31 Alexei A. Abrikosov

A classification result for Ricci-flat anti-self-dual asymptotically locally Euclidean 4-manifolds is obtained: they are either hyperk\"ahler (one of the gravitational instantons classified by Kronheimer), or they are a cyclic quotient of a…

Differential Geometry · Mathematics 2011-05-02 Evan P. Wright

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

Graphene kinks are topological states of buckled graphene membranes. We show that when a moving kink encounters a constriction, there are three general classes of behavior: reflection, trapping, and transmission. Overall, constriction is…

Mesoscale and Nanoscale Physics · Physics 2021-07-07 D. C. Nguyen , R. D. Yamaletdinov , Y. V. Pershin

Studied are moduli spaces of self dual or anti-self dual connections on noncommutative 4-manifolds, especially deformation quantization of compact spin Riemannian 4-manifolds and their isometry groups have 2-torus subgroup. Then such moduli…

Differential Geometry · Mathematics 2007-05-23 Hiroshi Takai

In this Letter, we address the {long-range interaction} between kinks and antikinks, as well as kinks and kinks, in $\varphi^{2n+4}$ field theories for $n>1$. The kink-antikink interaction is generically attractive, while the kink-kink…

High Energy Physics - Theory · Physics 2019-05-08 Ivan C. Christov , Robert J. Decker , A. Demirkaya , Vakhid A. Gani , P. G. Kevrekidis , Avinash Khare , Avadh Saxena

We study the full class of kinetically constrained models in arbitrary dimension and out of equilibrium, in the regime where the density $q$ of facilitating sites in the equilibrium measure (but not necessarily in the initial measure) is…

Probability · Mathematics 2024-05-29 Ivailo Hartarsky , Fabio Toninelli

We consider the interaction between instantons and anti-instantons in four-dimensional N=4 super-Yang-Mills theory at large N and large 't Hooft coupling as described by D-instantons via AdS/CFT duality. We give an estimate of the strength…

High Energy Physics - Theory · Physics 2009-10-31 J. L. F. Barbon , A. Pasquinucci

We review the physics of topological objects in QCD. Topics include: solitons, vortices, magnetic monopoles, instantons, (effective theories of) confinement.

High Energy Physics - Theory · Physics 2007-05-23 Gerard 't Hooft , Falk Bruckmann

In a dilute system of instantons and antiinstantons, the U$_{\rm A}$(1) and scale anomalies are shown to be directly related to the bulk susceptibility and compressibility of the system. Using $1/N_c$ (where $N_c$ is the number of colors)…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Kacir , M. Prakash , I. Zahed

Denote by MI(k) the moduli space of k-instanton bundles E of rank 2 on $\PP^3=\PP(V)$ and by $Z_k(E)$ the scheme of k-jumping lines. We prove that $[E]\in MI(k)$ is not stable for the action of SL(V) if $Z_k(E)\neq\emptyset$. Moreover $\dim…

Algebraic Geometry · Mathematics 2007-05-23 Laura Costa , Giorgio Ottaviani

We investigate the differential geometry of the moduli space of instantons on S^3 x S^1. Extending previous results, we show that a sigma-model with this target space can be expected to possess a large N=4 superconformal symmetry,…

High Energy Physics - Theory · Physics 2024-12-23 Edward Witten

Motivated by studies of the Greenberg-Hastings cellular automata (GHCA) as a caricature of excitable systems, in this paper we study kink-antikink dynamics in the perhaps simplest PDE model of excitable media given by the scalar reaction…

Analysis of PDEs · Mathematics 2020-12-02 Antoine Pauthier , Jens D. M. Rademacher , Dennis Ulbrich

We consider geodesics of infinite length and constant 4d dilaton in the (classical) hypermultiplet moduli space of type II Calabi-Yau compactifications. When approaching such infinite distance points, a large amount of D-instantons develop…

High Energy Physics - Theory · Physics 2019-09-04 Fernando Marchesano , Max Wiesner

We propose a toy model to reproduce the fractal structure of kink and antikink collisions on one topological sector of $\phi^6$ theory. Using the toy model, we investigate the missing bounce windows observed in the fractal structure, and…

High Energy Physics - Theory · Physics 2024-09-09 Lingxiao Long , Xiang Li , Yunguo Jiang

Direct numerical simulation of dense rigid body suspensions poses significant computational challenges. A popular approach to resolve collisions necessitates solving a linear complementary problem (LCP) per time step. Each matrix vector…

Optimization and Control · Mathematics 2026-04-14 Nicholas Rummel , Tyler Jensen , Stephen Becker , Eduardo Corona

On P3, we show that mathematical instantons in characteristic two are unobstructed. We produce upper bounds for the dimension of the moduli space of stable rank two bundles on P3 in characteristic two. In cases where there is a phenomenon…

alg-geom · Mathematics 2007-05-23 A. P. Rao
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