Strange and charm HVP contributions to the muon (g − 2) including QED corrections with twisted-mass fermions
Abstract We present a lattice calculation of the Hadronic Vacuum Polarization (HVP) contribution of the strange and charm quarks to the anomalous magnetic moment of the muon including leading-order electromagnetic corrections. We employ the gauge configurations generated by the European Twisted Mass...
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Online Access: | http://link.springer.com/article/10.1007/JHEP10(2017)157 |
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doaj-32dd68c922314885ab0a6dd85a6d66fd2020-11-24T23:43:30ZengSpringerOpenJournal of High Energy Physics1029-84792017-10-0120171013210.1007/JHEP10(2017)157Strange and charm HVP contributions to the muon (g − 2) including QED corrections with twisted-mass fermionsD. Giusti0V. Lubicz1G. Martinelli2F. Sanfilippo3S. Simula4on behalf of ETM collaborationDipartimento di Matematica e Fisica, Università di Roma TreDipartimento di Matematica e Fisica, Università di Roma TreDipartimento di Fisica, Università di Roma “La Sapienza” and INFN Sezione di RomaIstituto Nazionale di Fisica Nucleare, Sezione di Roma TreIstituto Nazionale di Fisica Nucleare, Sezione di Roma TreAbstract We present a lattice calculation of the Hadronic Vacuum Polarization (HVP) contribution of the strange and charm quarks to the anomalous magnetic moment of the muon including leading-order electromagnetic corrections. We employ the gauge configurations generated by the European Twisted Mass Collaboration (ETMC) with N f = 2 + 1 + 1 dynamical quarks at three values of the lattice spacing (a ≃ 0.062, 0.082, 0.089 fm) with pion masses in the range M π ≃ 210-450 MeV. The strange and charm quark masses are tuned at their physical values. Neglecting disconnected diagrams and after the extrapolations to the physical pion mass and to the continuum limit we obtain: a μ s (α em 2 ) = (53.1 ± 2.5) · 10− 10, a μ s (α em 3 ) = (−0.018 ± 0.011) · 10− 10 and a μ c (α em 2 ) = (14.75 ± 0.56) · 10− 10, a μ c (α em 3 ) = (−0.030 ± 0.013) · 10− 10 for the strange and charm contributions, respectively.http://link.springer.com/article/10.1007/JHEP10(2017)157Lattice field theory simulationQCD Phenomenology |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
D. Giusti V. Lubicz G. Martinelli F. Sanfilippo S. Simula on behalf of ETM collaboration |
spellingShingle |
D. Giusti V. Lubicz G. Martinelli F. Sanfilippo S. Simula on behalf of ETM collaboration Strange and charm HVP contributions to the muon (g − 2) including QED corrections with twisted-mass fermions Journal of High Energy Physics Lattice field theory simulation QCD Phenomenology |
author_facet |
D. Giusti V. Lubicz G. Martinelli F. Sanfilippo S. Simula on behalf of ETM collaboration |
author_sort |
D. Giusti |
title |
Strange and charm HVP contributions to the muon (g − 2) including QED corrections with twisted-mass fermions |
title_short |
Strange and charm HVP contributions to the muon (g − 2) including QED corrections with twisted-mass fermions |
title_full |
Strange and charm HVP contributions to the muon (g − 2) including QED corrections with twisted-mass fermions |
title_fullStr |
Strange and charm HVP contributions to the muon (g − 2) including QED corrections with twisted-mass fermions |
title_full_unstemmed |
Strange and charm HVP contributions to the muon (g − 2) including QED corrections with twisted-mass fermions |
title_sort |
strange and charm hvp contributions to the muon (g − 2) including qed corrections with twisted-mass fermions |
publisher |
SpringerOpen |
series |
Journal of High Energy Physics |
issn |
1029-8479 |
publishDate |
2017-10-01 |
description |
Abstract We present a lattice calculation of the Hadronic Vacuum Polarization (HVP) contribution of the strange and charm quarks to the anomalous magnetic moment of the muon including leading-order electromagnetic corrections. We employ the gauge configurations generated by the European Twisted Mass Collaboration (ETMC) with N f = 2 + 1 + 1 dynamical quarks at three values of the lattice spacing (a ≃ 0.062, 0.082, 0.089 fm) with pion masses in the range M π ≃ 210-450 MeV. The strange and charm quark masses are tuned at their physical values. Neglecting disconnected diagrams and after the extrapolations to the physical pion mass and to the continuum limit we obtain: a μ s (α em 2 ) = (53.1 ± 2.5) · 10− 10, a μ s (α em 3 ) = (−0.018 ± 0.011) · 10− 10 and a μ c (α em 2 ) = (14.75 ± 0.56) · 10− 10, a μ c (α em 3 ) = (−0.030 ± 0.013) · 10− 10 for the strange and charm contributions, respectively. |
topic |
Lattice field theory simulation QCD Phenomenology |
url |
http://link.springer.com/article/10.1007/JHEP10(2017)157 |
work_keys_str_mv |
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