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Related papers: Construction of Nahm data and BPS monopoles with c…

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We produce finite energy BPS monopoles with arbitrary prescribed symmetry breaking from a new class of Nahm data.

Differential Geometry · Mathematics 2025-08-15 Benoit Charbonneau , Ákos Nagy

This paper deals with static BPS monopoles in three dimensions which are periodic either in one direction (monopole chains) or two directions (monopole sheets). The Nahm construction of the simplest monopole chain is implemented…

High Energy Physics - Theory · Physics 2009-11-11 R. S. Ward

We show that the Higgs and gauge fields for a BPS monopole may be constructed directly from the spectral curve without having to solve the gauge constraint needed to obtain the Nahm data. The result is the analogue of the instanton result:…

High Energy Physics - Theory · Physics 2018-08-15 H. W. Braden , V. Z. Enolski

We study charge k SU(2) BPS monopoles which are symmetric under the cyclic group of order k. Approximate twistor data (spectral curves and Nahm data) is constructed using a new technique based upon a Painleve analysis of Nahm's equation…

High Energy Physics - Theory · Physics 2009-10-30 Paul Sutcliffe

BPS monopoles which are periodic in one of the spatial directions correspond, via a generalized Nahm transform, to solutions of the Hitchin equations on a cylinder. A one-parameter family of solutions of these equations, representing a…

High Energy Physics - Theory · Physics 2011-03-28 Derek Harland , R. S. Ward

We construct BPS solutions representing M2-M5 bound state in the ABJM action explicitly. They include the funnel type solutions and 't Hooft Polyakov monopole solutions. Furthermore, we give a one to one correspondence between the solutions…

High Energy Physics - Theory · Physics 2013-05-30 Tomoki Nosaka , Seiji Terashima

BPS monopoles on $\mathbb{R}^2\times S^1$ correspond, via the generalized Nahm transform, to certain solutions of the Hitchin equations on the cylinder $\mathbb{R}\times S^1$. The moduli space M of two monopoles with their centre-of-mass…

High Energy Physics - Theory · Physics 2014-07-14 Rafael Maldonado , R S Ward

Starting from Nahm's equations, we explore BPS magnetic monopoles in the Yang-Mills Higgs theory of gauge group $Sp(4)$ which is broken to $SU(2)\times U(1)$. A family of BPS field configurations with purely Abelian magnetic charge describe…

High Energy Physics - Theory · Physics 2016-08-25 Kimyeong Lee , Changhai Lu

Certain spontaneously broken gauge theories contain massless magnetic monopoles. These are realized classically as clouds of non-Abelian fields surrounding one or more massive monopoles. In order to gain a better understanding of these…

High Energy Physics - Theory · Physics 2009-11-07 Conor J. Houghton , Erick J. Weinberg

We discuss $SU(2)$ Bogomolny monopoles of arbitrary charge $k$ invariant under various symmetry groups. The analysis is largely in terms of the spectral curves, the rational maps, and the Nahm equations associated with monopoles. We…

dg-ga · Mathematics 2016-08-31 N. J. Hitchin , N. S. Manton , M. K. Murray

We investigate BPS equations which determine the configuration of an M2-M5 bound state preserving half of the supersymmetries in the ABJM theory. We argue that the BPS equations are classically integrable, showing that they admit a Lax…

High Energy Physics - Theory · Physics 2015-06-16 Kazuhiro Sakai , Seiji Terashima

For N>2 we present static monopole solutions of the second order SU(N) BPS Yang-Mills-Higgs equations which are not solutions of the first order Bogomolny equations. These spherically symmetric solutions may be interpreted as monopole…

High Energy Physics - Theory · Physics 2010-11-19 Theodora Ioannidou , Paul M. Sutcliffe

We consider singly periodic solutions to the SU(2) Bogomolny equations and use the Nahm transform to generate a class of monopoles of charge k>2, thereby extending known results for lower charge chains. Some simple scattering processes are…

High Energy Physics - Theory · Physics 2013-11-26 Rafael Maldonado

We formulate a correspondence between SU(2) monopole chains and ``spectral data'', consisting of curves in $\mathbb{CP}^1\times\mathbb{CP}^1$ equipped with parabolic line bundles. This is the analogue for monopole chains of Donaldson's…

Differential Geometry · Mathematics 2021-05-25 Derek Harland

We construct a spherically symmetric noncommutative space in three dimensions by foliating the space with concentric fuzzy spheres. We show how to construct a gauge theory in this space and in particular we derive the noncommutative version…

High Energy Physics - Theory · Physics 2009-11-11 E. F. Moreno

The mass of 1/4-BPS dyonic configurations in N=4 D=4 supersymmetric Yang-Mills theories is calculated within the Nahm formulation. The SU(3) example, with two massive monopoles and one massless monopole, is considered in detail. In this…

High Energy Physics - Theory · Physics 2009-10-31 Conor Houghton , Kimyeong Lee

Our approach to define monopoles is twistorial and we start by developing the twistor theory of R^5, which is an analogue of the twistor theory for R^3 developed by Hitchin. Using this, we describe a Hitchin-Ward transform for R^5, that…

Differential Geometry · Mathematics 2016-10-04 Rodrigo Pires dos Santos

We consider a variant of the Georgi Glashow model in the BPS limit, augmented by a higher derivative Skyrme-like term, which is the simplest YMH model that can support monopole bound states. The spherically symetric solutions are studied…

High Energy Physics - Theory · Physics 2008-11-26 Y. Brihaye , J. Burzlaff , D. H. Tchrakian

A deformed Nahm equation for the BPS equation in the noncommutative N=4 supersymmetric U(2) Yang-Mills theory is obtained. Using this, we constructed explicitly a monopole solution of the noncommutative BPS equation to the linear order of…

High Energy Physics - Theory · Physics 2015-06-26 Dongsu Bak

We study Bogomolny equations on $R^2\times S^1$. Although they do not admit nontrivial finite-energy solutions, we show that there are interesting infinite-energy solutions with Higgs field growing logarithmically at infinity. We call these…

High Energy Physics - Theory · Physics 2009-10-31 Sergey A. Cherkis , Anton Kapustin
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