Sigma-model limit of Yang-Mills instantons in higher dimensions

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OriginalspracheEnglisch
Seiten (von - bis)361-373
Seitenumfang13
FachzeitschriftNuclear Physics B
Jahrgang894
PublikationsstatusVeröffentlicht - 2015

Abstract

We consider the Hermitian Yang-Mills (instanton) equations for connections on vector bundles over a 2n-dimensional Kähler manifold X which is a product Y×. Z of p- and q-dimensional Riemannian manifold Y and Z with p+. q=2. n. We show that in the adiabatic limit, when the metric in the Z direction is scaled down, the gauge instanton equations on Y×. Z become sigma-model instanton equations for maps from Y to the moduli space M (target space) of gauge instantons on Z if q≥. 4. For q<. 4 we get maps from Y to the moduli space M of flat connections on Z. Thus, the Yang-Mills instantons on Y×. Z converge to sigma-model instantons on Y while Z shrinks to a point. Put differently, for small volume of Z, sigma-model instantons on Y with target space M approximate Yang-Mills instantons on Y×. Z.

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Sigma-model limit of Yang-Mills instantons in higher dimensions. / Deser, Andreas; Lechtenfeld, Olaf; Popov, Alexander D.
in: Nuclear Physics B, Jahrgang 894, 2015, S. 361-373.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Deser A, Lechtenfeld O, Popov AD. Sigma-model limit of Yang-Mills instantons in higher dimensions. Nuclear Physics B. 2015;894:361-373. doi: 10.1016/j.nuclphysb.2015.03.009
Deser, Andreas ; Lechtenfeld, Olaf ; Popov, Alexander D. / Sigma-model limit of Yang-Mills instantons in higher dimensions. in: Nuclear Physics B. 2015 ; Jahrgang 894. S. 361-373.
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title = "Sigma-model limit of Yang-Mills instantons in higher dimensions",
abstract = "We consider the Hermitian Yang-Mills (instanton) equations for connections on vector bundles over a 2n-dimensional K{\"a}hler manifold X which is a product Y×. Z of p- and q-dimensional Riemannian manifold Y and Z with p+. q=2. n. We show that in the adiabatic limit, when the metric in the Z direction is scaled down, the gauge instanton equations on Y×. Z become sigma-model instanton equations for maps from Y to the moduli space M (target space) of gauge instantons on Z if q≥. 4. For q<. 4 we get maps from Y to the moduli space M of flat connections on Z. Thus, the Yang-Mills instantons on Y×. Z converge to sigma-model instantons on Y while Z shrinks to a point. Put differently, for small volume of Z, sigma-model instantons on Y with target space M approximate Yang-Mills instantons on Y×. Z.",
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AU - Deser, Andreas

AU - Lechtenfeld, Olaf

AU - Popov, Alexander D.

N1 - Funding Information: This work was partially supported by the Deutsche Forschungsgemeinschaft grant LE 838/13 . Publisher Copyright: © 2015 The Authors. Copyright: Copyright 2018 Elsevier B.V., All rights reserved.

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N2 - We consider the Hermitian Yang-Mills (instanton) equations for connections on vector bundles over a 2n-dimensional Kähler manifold X which is a product Y×. Z of p- and q-dimensional Riemannian manifold Y and Z with p+. q=2. n. We show that in the adiabatic limit, when the metric in the Z direction is scaled down, the gauge instanton equations on Y×. Z become sigma-model instanton equations for maps from Y to the moduli space M (target space) of gauge instantons on Z if q≥. 4. For q<. 4 we get maps from Y to the moduli space M of flat connections on Z. Thus, the Yang-Mills instantons on Y×. Z converge to sigma-model instantons on Y while Z shrinks to a point. Put differently, for small volume of Z, sigma-model instantons on Y with target space M approximate Yang-Mills instantons on Y×. Z.

AB - We consider the Hermitian Yang-Mills (instanton) equations for connections on vector bundles over a 2n-dimensional Kähler manifold X which is a product Y×. Z of p- and q-dimensional Riemannian manifold Y and Z with p+. q=2. n. We show that in the adiabatic limit, when the metric in the Z direction is scaled down, the gauge instanton equations on Y×. Z become sigma-model instanton equations for maps from Y to the moduli space M (target space) of gauge instantons on Z if q≥. 4. For q<. 4 we get maps from Y to the moduli space M of flat connections on Z. Thus, the Yang-Mills instantons on Y×. Z converge to sigma-model instantons on Y while Z shrinks to a point. Put differently, for small volume of Z, sigma-model instantons on Y with target space M approximate Yang-Mills instantons on Y×. Z.

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