Constraining CP-violating electron-gluonic operators

Abstract We present an analysis of constraints on two types of CP-odd electron-gluonic operators (ēiγ 5 e)G μν a G aμν and e ¯ e G μ ν a G ∼ a μ ν $$ \left(\overline{e}e\right){G}_{\mu \nu}^a{\overset{\sim }{G}}^{a\mu \nu } $$ from current and future electric dipole moment (EDM) experiments. The rec...

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Main Authors: Kingman Cheung, Wai-Yee Keung, Ying-nan Mao, Chen Zhang
Format: Article
Language:English
Published: SpringerOpen 2019-07-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP07(2019)074
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spelling doaj-acd6982e1ed14e67be5df11e5d7cb6f22020-11-25T03:02:23ZengSpringerOpenJournal of High Energy Physics1029-84792019-07-012019712210.1007/JHEP07(2019)074Constraining CP-violating electron-gluonic operatorsKingman Cheung0Wai-Yee Keung1Ying-nan Mao2Chen Zhang3Physics Division, National Center for Theoretical SciencesDepartment of Physics, University of Illinois at ChicagoPhysics Division, National Center for Theoretical SciencesPhysics Division, National Center for Theoretical SciencesAbstract We present an analysis of constraints on two types of CP-odd electron-gluonic operators (ēiγ 5 e)G μν a G aμν and e ¯ e G μ ν a G ∼ a μ ν $$ \left(\overline{e}e\right){G}_{\mu \nu}^a{\overset{\sim }{G}}^{a\mu \nu } $$ from current and future electric dipole moment (EDM) experiments. The recent result from the ACME experiment using ThO molecules is used to derive an impressive lower bound on the effective scale for (ēiγ 5 e)G μν a G aμν at 8 TeV, assuming a QCD one-loop factor and no helicity suppression from new physics. One interesting aspect is that (ēiγ 5 e)G μν a G aμν contributes to the observable EDM in ThO experiment mainly through CP-odd electron-nucleon interaction rather than direct electron EDM which arises from three-loop running and matching. For e ¯ e G μ ν a G ∼ a μ ν $$ \left(\overline{e}e\right){G}_{\mu \nu}^a{\overset{\sim }{G}}^{a\mu \nu } $$ the current bound is much weaker and suffers from large uncertainties. We also discuss the QCD running and matching for the CP-odd electron-gluonic operators and give an estimate of the relevant nucleon matrix elements and uncertainties that are needed in the calculation.http://link.springer.com/article/10.1007/JHEP07(2019)074CP violationBeyond Standard ModelDiscrete SymmetriesEffective Field Theories
collection DOAJ
language English
format Article
sources DOAJ
author Kingman Cheung
Wai-Yee Keung
Ying-nan Mao
Chen Zhang
spellingShingle Kingman Cheung
Wai-Yee Keung
Ying-nan Mao
Chen Zhang
Constraining CP-violating electron-gluonic operators
Journal of High Energy Physics
CP violation
Beyond Standard Model
Discrete Symmetries
Effective Field Theories
author_facet Kingman Cheung
Wai-Yee Keung
Ying-nan Mao
Chen Zhang
author_sort Kingman Cheung
title Constraining CP-violating electron-gluonic operators
title_short Constraining CP-violating electron-gluonic operators
title_full Constraining CP-violating electron-gluonic operators
title_fullStr Constraining CP-violating electron-gluonic operators
title_full_unstemmed Constraining CP-violating electron-gluonic operators
title_sort constraining cp-violating electron-gluonic operators
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2019-07-01
description Abstract We present an analysis of constraints on two types of CP-odd electron-gluonic operators (ēiγ 5 e)G μν a G aμν and e ¯ e G μ ν a G ∼ a μ ν $$ \left(\overline{e}e\right){G}_{\mu \nu}^a{\overset{\sim }{G}}^{a\mu \nu } $$ from current and future electric dipole moment (EDM) experiments. The recent result from the ACME experiment using ThO molecules is used to derive an impressive lower bound on the effective scale for (ēiγ 5 e)G μν a G aμν at 8 TeV, assuming a QCD one-loop factor and no helicity suppression from new physics. One interesting aspect is that (ēiγ 5 e)G μν a G aμν contributes to the observable EDM in ThO experiment mainly through CP-odd electron-nucleon interaction rather than direct electron EDM which arises from three-loop running and matching. For e ¯ e G μ ν a G ∼ a μ ν $$ \left(\overline{e}e\right){G}_{\mu \nu}^a{\overset{\sim }{G}}^{a\mu \nu } $$ the current bound is much weaker and suffers from large uncertainties. We also discuss the QCD running and matching for the CP-odd electron-gluonic operators and give an estimate of the relevant nucleon matrix elements and uncertainties that are needed in the calculation.
topic CP violation
Beyond Standard Model
Discrete Symmetries
Effective Field Theories
url http://link.springer.com/article/10.1007/JHEP07(2019)074
work_keys_str_mv AT kingmancheung constrainingcpviolatingelectrongluonicoperators
AT waiyeekeung constrainingcpviolatingelectrongluonicoperators
AT yingnanmao constrainingcpviolatingelectrongluonicoperators
AT chenzhang constrainingcpviolatingelectrongluonicoperators
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