Two-loop massive quark jet functions in SCET

Abstract We calculate the O( α s 2 $$ {\alpha}_s^2 $$ ) corrections to the primary massive quark jet functions in Soft-Collinear Effective Theory (SCET). They are an important ingredient in factorized predictions for inclusive jet mass cross sections initiated by massive quarks emerging from a hard...

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Main Authors: André H. Hoang, Christopher Lepenik, Maximilian Stahlhofen
Format: Article
Language:English
Published: SpringerOpen 2019-08-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP08(2019)112
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spelling doaj-54edddd4685e4f47a70e149b3b92be9d2020-11-25T03:56:50ZengSpringerOpenJournal of High Energy Physics1029-84792019-08-012019816010.1007/JHEP08(2019)112Two-loop massive quark jet functions in SCETAndré H. Hoang0Christopher Lepenik1Maximilian Stahlhofen2University of Vienna, Faculty of PhysicsUniversity of Vienna, Faculty of PhysicsPRISMA Cluster of Excellence, Johannes Gutenberg UniversityAbstract We calculate the O( α s 2 $$ {\alpha}_s^2 $$ ) corrections to the primary massive quark jet functions in Soft-Collinear Effective Theory (SCET). They are an important ingredient in factorized predictions for inclusive jet mass cross sections initiated by massive quarks emerging from a hard interaction with smooth quark mass dependence. Due to the effects coming from the secondary production of massive quark-antiquark pairs there are two options to define the SCET jet function, which we call universal and mass mode jet functions. They are related to whether or not a soft mass mode (zero) bin subtraction is applied for the secondary massive quark contributions and differ in particular concerning the infrared behavior for vanishing quark mass. We advocate that a useful alternative to the common zero-bin subtraction concept is to define the SCET jet functions through subtractions related to collinear-soft matrix elements. This avoids the need to impose additional power counting arguments as required for zero-bin subtractions. We demonstrate how the two SCET jet function definitions may be used in the context of two recently developed factorization approaches to treat secondary massive quark effects. We clarify the relation between these approaches and in which way they are equivalent. Our two-loop calculation involves interesting technical subtleties related to spurious rapidity divergences and infrared regularization in the presence of massive quarks.http://link.springer.com/article/10.1007/JHEP08(2019)112JetsNLO Computations
collection DOAJ
language English
format Article
sources DOAJ
author André H. Hoang
Christopher Lepenik
Maximilian Stahlhofen
spellingShingle André H. Hoang
Christopher Lepenik
Maximilian Stahlhofen
Two-loop massive quark jet functions in SCET
Journal of High Energy Physics
Jets
NLO Computations
author_facet André H. Hoang
Christopher Lepenik
Maximilian Stahlhofen
author_sort André H. Hoang
title Two-loop massive quark jet functions in SCET
title_short Two-loop massive quark jet functions in SCET
title_full Two-loop massive quark jet functions in SCET
title_fullStr Two-loop massive quark jet functions in SCET
title_full_unstemmed Two-loop massive quark jet functions in SCET
title_sort two-loop massive quark jet functions in scet
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2019-08-01
description Abstract We calculate the O( α s 2 $$ {\alpha}_s^2 $$ ) corrections to the primary massive quark jet functions in Soft-Collinear Effective Theory (SCET). They are an important ingredient in factorized predictions for inclusive jet mass cross sections initiated by massive quarks emerging from a hard interaction with smooth quark mass dependence. Due to the effects coming from the secondary production of massive quark-antiquark pairs there are two options to define the SCET jet function, which we call universal and mass mode jet functions. They are related to whether or not a soft mass mode (zero) bin subtraction is applied for the secondary massive quark contributions and differ in particular concerning the infrared behavior for vanishing quark mass. We advocate that a useful alternative to the common zero-bin subtraction concept is to define the SCET jet functions through subtractions related to collinear-soft matrix elements. This avoids the need to impose additional power counting arguments as required for zero-bin subtractions. We demonstrate how the two SCET jet function definitions may be used in the context of two recently developed factorization approaches to treat secondary massive quark effects. We clarify the relation between these approaches and in which way they are equivalent. Our two-loop calculation involves interesting technical subtleties related to spurious rapidity divergences and infrared regularization in the presence of massive quarks.
topic Jets
NLO Computations
url http://link.springer.com/article/10.1007/JHEP08(2019)112
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