Wilson loop of the heterotic sigma model and the sv-map

The single-valued projection (sv) is a relation between scattering amplitudes of gauge bosons in heterotic and open superstring theories. Recently we have studied sv from the aspect of nonlinear sigma models [1], where the gauge physics of open string sigma model is under the Wilson loop representat...

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Main Author: Wei Fan
Format: Article
Language:English
Published: Elsevier 2018-11-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321318302803
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spelling doaj-9500c93fd94b4233a967bf2407190bea2020-11-24T21:47:53ZengElsevierNuclear Physics B0550-32132018-11-01936615637Wilson loop of the heterotic sigma model and the sv-mapWei Fan0Department of Physics, Northeastern University, Boston, MA 02115, USA; Institute of Theoretical Physics, Faculty of Physics, University of Warsaw, Poland; Correspondence to: Department of Physics, Northeastern University, Boston, MA 02115, USA.The single-valued projection (sv) is a relation between scattering amplitudes of gauge bosons in heterotic and open superstring theories. Recently we have studied sv from the aspect of nonlinear sigma models [1], where the gauge physics of open string sigma model is under the Wilson loop representation but the gauge physics of heterotic string sigma model is under the fermionic representation since the Wilson loop representation is absent in the heterotic case. There we showed that the sv comes from a sum of six radial orderings of heterotic vertices on the complex plane. In this paper, we propose a Wilson loop representation for the heterotic case and using the Wilson loop representation to show that sv comes from a sum of two opposite-directed contours of the heterotic sigma model. We firstly prove that the Wilson loop is the exact propagator of the fermion field that carry the gauge physics of the heterotic string in the fermionic representation. Then we construct the action of the heterotic string sigma model in terms of the Wilson loop, by exploring the geometry of the Wilson loop and by generalizing the nonabelian Stokes's theorem [2–4] to the fermionic case. After that, we compute some three loop and four loop diagrams as an example, to show how the sv for ζ2 and ζ3 arises from a sum of the contours of the Wilson loop. Finally we conjecture that this sum of contours of the Wilson loop is the mechanism behind the sv for general cases.http://www.sciencedirect.com/science/article/pii/S0550321318302803
collection DOAJ
language English
format Article
sources DOAJ
author Wei Fan
spellingShingle Wei Fan
Wilson loop of the heterotic sigma model and the sv-map
Nuclear Physics B
author_facet Wei Fan
author_sort Wei Fan
title Wilson loop of the heterotic sigma model and the sv-map
title_short Wilson loop of the heterotic sigma model and the sv-map
title_full Wilson loop of the heterotic sigma model and the sv-map
title_fullStr Wilson loop of the heterotic sigma model and the sv-map
title_full_unstemmed Wilson loop of the heterotic sigma model and the sv-map
title_sort wilson loop of the heterotic sigma model and the sv-map
publisher Elsevier
series Nuclear Physics B
issn 0550-3213
publishDate 2018-11-01
description The single-valued projection (sv) is a relation between scattering amplitudes of gauge bosons in heterotic and open superstring theories. Recently we have studied sv from the aspect of nonlinear sigma models [1], where the gauge physics of open string sigma model is under the Wilson loop representation but the gauge physics of heterotic string sigma model is under the fermionic representation since the Wilson loop representation is absent in the heterotic case. There we showed that the sv comes from a sum of six radial orderings of heterotic vertices on the complex plane. In this paper, we propose a Wilson loop representation for the heterotic case and using the Wilson loop representation to show that sv comes from a sum of two opposite-directed contours of the heterotic sigma model. We firstly prove that the Wilson loop is the exact propagator of the fermion field that carry the gauge physics of the heterotic string in the fermionic representation. Then we construct the action of the heterotic string sigma model in terms of the Wilson loop, by exploring the geometry of the Wilson loop and by generalizing the nonabelian Stokes's theorem [2–4] to the fermionic case. After that, we compute some three loop and four loop diagrams as an example, to show how the sv for ζ2 and ζ3 arises from a sum of the contours of the Wilson loop. Finally we conjecture that this sum of contours of the Wilson loop is the mechanism behind the sv for general cases.
url http://www.sciencedirect.com/science/article/pii/S0550321318302803
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