Yang-Mills instantons and dyons on group manifolds

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Original languageEnglish
Pages (from-to)91-94
Number of pages4
JournalPhysics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
Volume670
Issue number1
Publication statusPublished - 4 Dec 2008

Abstract

We consider Euclidean SU (N) Yang-Mills theory on the space G × R, where G is a compact semisimple Lie group, and introduce first-order BPS-type equations which imply the full Yang-Mills equations. For gauge fields invariant under the adjoint G-action these BPS equations reduce to first-order matrix equations, to which we give instanton solutions. In the case of G = SU (2) ≅ S3, our matrix equations are recast as Nahm equations, and a further algebraic reduction to the Toda chain equations is presented and solved for the SU(3) example. Finally, we change the metric on G × R to Minkowski and construct finite-energy dyon-type Yang-Mills solutions. The special case of G = SU (2) × SU (2) may be used in heterotic flux compactifications.

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Yang-Mills instantons and dyons on group manifolds. / Ivanova, Tatiana A.; Lechtenfeld, Olaf.
In: Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics, Vol. 670, No. 1, 04.12.2008, p. 91-94.

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abstract = "We consider Euclidean SU (N) Yang-Mills theory on the space G × R, where G is a compact semisimple Lie group, and introduce first-order BPS-type equations which imply the full Yang-Mills equations. For gauge fields invariant under the adjoint G-action these BPS equations reduce to first-order matrix equations, to which we give instanton solutions. In the case of G = SU (2) ≅ S3, our matrix equations are recast as Nahm equations, and a further algebraic reduction to the Toda chain equations is presented and solved for the SU(3) example. Finally, we change the metric on G × R to Minkowski and construct finite-energy dyon-type Yang-Mills solutions. The special case of G = SU (2) × SU (2) may be used in heterotic flux compactifications.",
author = "Ivanova, {Tatiana A.} and Olaf Lechtenfeld",
note = "Funding Information: The authors are grateful to A.D. Popov for fruitful discussions and useful comments. T.A.I. acknowledges the Heisenberg–Landau program and the Russian Foundation for Basic Research (grant 06-01-00627-a) for partial support and the Institut f{\"u}r Theoretische Physik der Leibniz Universit{\"a}t Hannover for its hospitality. The work of O.L. is partially supported by the Deutsche Forschungsgemeinschaft. Copyright: Copyright 2008 Elsevier B.V., All rights reserved.",
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TY - JOUR

T1 - Yang-Mills instantons and dyons on group manifolds

AU - Ivanova, Tatiana A.

AU - Lechtenfeld, Olaf

N1 - Funding Information: The authors are grateful to A.D. Popov for fruitful discussions and useful comments. T.A.I. acknowledges the Heisenberg–Landau program and the Russian Foundation for Basic Research (grant 06-01-00627-a) for partial support and the Institut für Theoretische Physik der Leibniz Universität Hannover for its hospitality. The work of O.L. is partially supported by the Deutsche Forschungsgemeinschaft. Copyright: Copyright 2008 Elsevier B.V., All rights reserved.

PY - 2008/12/4

Y1 - 2008/12/4

N2 - We consider Euclidean SU (N) Yang-Mills theory on the space G × R, where G is a compact semisimple Lie group, and introduce first-order BPS-type equations which imply the full Yang-Mills equations. For gauge fields invariant under the adjoint G-action these BPS equations reduce to first-order matrix equations, to which we give instanton solutions. In the case of G = SU (2) ≅ S3, our matrix equations are recast as Nahm equations, and a further algebraic reduction to the Toda chain equations is presented and solved for the SU(3) example. Finally, we change the metric on G × R to Minkowski and construct finite-energy dyon-type Yang-Mills solutions. The special case of G = SU (2) × SU (2) may be used in heterotic flux compactifications.

AB - We consider Euclidean SU (N) Yang-Mills theory on the space G × R, where G is a compact semisimple Lie group, and introduce first-order BPS-type equations which imply the full Yang-Mills equations. For gauge fields invariant under the adjoint G-action these BPS equations reduce to first-order matrix equations, to which we give instanton solutions. In the case of G = SU (2) ≅ S3, our matrix equations are recast as Nahm equations, and a further algebraic reduction to the Toda chain equations is presented and solved for the SU(3) example. Finally, we change the metric on G × R to Minkowski and construct finite-energy dyon-type Yang-Mills solutions. The special case of G = SU (2) × SU (2) may be used in heterotic flux compactifications.

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JO - Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics

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