The Bremsstrahlung function of N $$ \mathcal{N} $$ = 2 SCQCD

Abstract For SU(N) superconformal QCD we perform a three-loop calculation of the cusp anomalous dimension for a generalized Maldacena-Wilson operator, using HQET formalism. We obtain an expression that is valid at generic geometric and internal angles and finite gauge group rank N. For equal and opp...

Full description

Bibliographic Details
Main Authors: Carolina Gomez, Andrea Mauri, Silvia Penati
Format: Article
Language:English
Published: SpringerOpen 2019-03-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP03(2019)122
id doaj-2e122ca3ff31439fae81c2c2ffe90ef5
record_format Article
spelling doaj-2e122ca3ff31439fae81c2c2ffe90ef52020-11-25T02:01:35ZengSpringerOpenJournal of High Energy Physics1029-84792019-03-012019312610.1007/JHEP03(2019)122The Bremsstrahlung function of N $$ \mathcal{N} $$ = 2 SCQCDCarolina Gomez0Andrea Mauri1Silvia Penati2Dipartimento di Fisica, Università degli studi di Milano-BicoccaDipartimento di Fisica, Università degli studi di Milano-BicoccaDipartimento di Fisica, Università degli studi di Milano-BicoccaAbstract For SU(N) superconformal QCD we perform a three-loop calculation of the cusp anomalous dimension for a generalized Maldacena-Wilson operator, using HQET formalism. We obtain an expression that is valid at generic geometric and internal angles and finite gauge group rank N. For equal and opposite angles this expression vanishes, proving that at these points the cusp becomes BPS. From its small angle expansion we derive the corresponding Bremsstrahlung function at three loops, matching the matrix model prediction given in terms of derivatives of the Wilson loop on the ellipsoid. Finally, we discuss possible scenarios at higher loops, with respect to the existence of a universal effective coupling in an integrable subsector of the model.http://link.springer.com/article/10.1007/JHEP03(2019)122Extended SupersymmetryMatrix ModelsSupersymmetric Gauge TheoryWilson, ’t Hooft and Polyakov loops
collection DOAJ
language English
format Article
sources DOAJ
author Carolina Gomez
Andrea Mauri
Silvia Penati
spellingShingle Carolina Gomez
Andrea Mauri
Silvia Penati
The Bremsstrahlung function of N $$ \mathcal{N} $$ = 2 SCQCD
Journal of High Energy Physics
Extended Supersymmetry
Matrix Models
Supersymmetric Gauge Theory
Wilson, ’t Hooft and Polyakov loops
author_facet Carolina Gomez
Andrea Mauri
Silvia Penati
author_sort Carolina Gomez
title The Bremsstrahlung function of N $$ \mathcal{N} $$ = 2 SCQCD
title_short The Bremsstrahlung function of N $$ \mathcal{N} $$ = 2 SCQCD
title_full The Bremsstrahlung function of N $$ \mathcal{N} $$ = 2 SCQCD
title_fullStr The Bremsstrahlung function of N $$ \mathcal{N} $$ = 2 SCQCD
title_full_unstemmed The Bremsstrahlung function of N $$ \mathcal{N} $$ = 2 SCQCD
title_sort bremsstrahlung function of n $$ \mathcal{n} $$ = 2 scqcd
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2019-03-01
description Abstract For SU(N) superconformal QCD we perform a three-loop calculation of the cusp anomalous dimension for a generalized Maldacena-Wilson operator, using HQET formalism. We obtain an expression that is valid at generic geometric and internal angles and finite gauge group rank N. For equal and opposite angles this expression vanishes, proving that at these points the cusp becomes BPS. From its small angle expansion we derive the corresponding Bremsstrahlung function at three loops, matching the matrix model prediction given in terms of derivatives of the Wilson loop on the ellipsoid. Finally, we discuss possible scenarios at higher loops, with respect to the existence of a universal effective coupling in an integrable subsector of the model.
topic Extended Supersymmetry
Matrix Models
Supersymmetric Gauge Theory
Wilson, ’t Hooft and Polyakov loops
url http://link.springer.com/article/10.1007/JHEP03(2019)122
work_keys_str_mv AT carolinagomez thebremsstrahlungfunctionofnmathcaln2scqcd
AT andreamauri thebremsstrahlungfunctionofnmathcaln2scqcd
AT silviapenati thebremsstrahlungfunctionofnmathcaln2scqcd
AT carolinagomez bremsstrahlungfunctionofnmathcaln2scqcd
AT andreamauri bremsstrahlungfunctionofnmathcaln2scqcd
AT silviapenati bremsstrahlungfunctionofnmathcaln2scqcd
_version_ 1724956849934958592