Top Quark Mass Calibration for Monte Carlo Event Generators
The most precise top quark mass measurements use kinematic reconstruction methods, determining the top mass parameter of a Monte Carlo event generator m$MC\atop{t}$. Because of hadronization and parton-shower dynamics, relating m$MC\atop{t}$ to a field theory mass is difficult. Here, we present a ca...
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Veröffentlicht in: | Physical review letters 2016-11, Vol.117 (23) |
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creator | Butenschoen, Mathias Dehnadi, Bahman Hoang, André H. Mateu, Vicent Preisser, Moritz Stewart, Iain W. |
description | The most precise top quark mass measurements use kinematic reconstruction methods, determining the top mass parameter of a Monte Carlo event generator m$MC\atop{t}$. Because of hadronization and parton-shower dynamics, relating m$MC\atop{t}$ to a field theory mass is difficult. Here, we present a calibration procedure to determine this relation using hadron level QCD predictions for observables with kinematic mass sensitivity. Fitting e+e-2-jettiness calculations at next-to-leading-logarithmic and next-to-next-to-leading-logarithmic order to PYTHIA 8.205, m$MC\atop{t}$ differs from the pole mass by 900 and 600 MeV, respectively, and agrees with the MSR mass within uncertainties, m$MC\atop{t}$ ≃ m$MSR\atop{t,1 GeV}$. |
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Because of hadronization and parton-shower dynamics, relating m$MC\atop{t}$ to a field theory mass is difficult. Here, we present a calibration procedure to determine this relation using hadron level QCD predictions for observables with kinematic mass sensitivity. Fitting e+e-2-jettiness calculations at next-to-leading-logarithmic and next-to-next-to-leading-logarithmic order to PYTHIA 8.205, m$MC\atop{t}$ differs from the pole mass by 900 and 600 MeV, respectively, and agrees with the MSR mass within uncertainties, m$MC\atop{t}$ ≃ m$MSR\atop{t,1 GeV}$.</description><identifier>ISSN: 0031-9007</identifier><identifier>EISSN: 1079-7114</identifier><language>eng</language><publisher>United States: American Physical Society (APS)</publisher><subject>CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS ; Heavy quark effective theory ; mass ; Perturbative QCD ; Quark & gluon jets ; Resummation methods ; Top Quark</subject><ispartof>Physical review letters, 2016-11, Vol.117 (23)</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881</link.rule.ids><backlink>$$Uhttps://www.osti.gov/servlets/purl/1424975$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Butenschoen, Mathias</creatorcontrib><creatorcontrib>Dehnadi, Bahman</creatorcontrib><creatorcontrib>Hoang, André H.</creatorcontrib><creatorcontrib>Mateu, Vicent</creatorcontrib><creatorcontrib>Preisser, Moritz</creatorcontrib><creatorcontrib>Stewart, Iain W.</creatorcontrib><creatorcontrib>Massachusetts Inst. of Technology (MIT), Cambridge, MA (United States)</creatorcontrib><title>Top Quark Mass Calibration for Monte Carlo Event Generators</title><title>Physical review letters</title><description>The most precise top quark mass measurements use kinematic reconstruction methods, determining the top mass parameter of a Monte Carlo event generator m$MC\atop{t}$. Because of hadronization and parton-shower dynamics, relating m$MC\atop{t}$ to a field theory mass is difficult. Here, we present a calibration procedure to determine this relation using hadron level QCD predictions for observables with kinematic mass sensitivity. 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Because of hadronization and parton-shower dynamics, relating m$MC\atop{t}$ to a field theory mass is difficult. Here, we present a calibration procedure to determine this relation using hadron level QCD predictions for observables with kinematic mass sensitivity. Fitting e+e-2-jettiness calculations at next-to-leading-logarithmic and next-to-next-to-leading-logarithmic order to PYTHIA 8.205, m$MC\atop{t}$ differs from the pole mass by 900 and 600 MeV, respectively, and agrees with the MSR mass within uncertainties, m$MC\atop{t}$ ≃ m$MSR\atop{t,1 GeV}$.</abstract><cop>United States</cop><pub>American Physical Society (APS)</pub><oa>free_for_read</oa></addata></record> |
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subjects | CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS Heavy quark effective theory mass Perturbative QCD Quark & gluon jets Resummation methods Top Quark |
title | Top Quark Mass Calibration for Monte Carlo Event Generators |
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