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 (e.m.) 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 ($a simeq 0.062, 0.082, 0.089$ fm) with pion masses in the range $M_pi simeq 210 - 450$ 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: $a_mu^s(alpha_em^2) = (53.1 pm 2.5) cdot 10^-10$, $a_mu^s(alpha_em^3) = (-0.018 pm 0.011) cdot 10^-10$ and $a_mu^c(alpha_em^2) = (14.75 pm 0.56) cdot 10^-10$, $a_mu^c(alpha_em^3) = (-0.030 pm 0.013) cdot 10^-10$ for the strange and charm contributions, respectively.

HVP contributions to the muon (g -2) including QED corrections with twisted-mass fermions / Giusti, D.; Lubicz, V.; Martinelli, G.; Sanfilippo, F.; Simula, S.. - In: EPJ WEB OF CONFERENCES. - ISSN 2100-014X. - 175:(2018), p. 06006. (Intervento presentato al convegno 35th International Symposium on Lattice Field Theory, Lattice 2017 tenutosi a Exhibition and Conference Centre in Granada, esp) [10.1051/epjconf/201817506006].

HVP contributions to the muon (g -2) including QED corrections with twisted-mass fermions

Martinelli G.;
2018

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 (e.m.) 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 ($a simeq 0.062, 0.082, 0.089$ fm) with pion masses in the range $M_pi simeq 210 - 450$ 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: $a_mu^s(alpha_em^2) = (53.1 pm 2.5) cdot 10^-10$, $a_mu^s(alpha_em^3) = (-0.018 pm 0.011) cdot 10^-10$ and $a_mu^c(alpha_em^2) = (14.75 pm 0.56) cdot 10^-10$, $a_mu^c(alpha_em^3) = (-0.030 pm 0.013) cdot 10^-10$ for the strange and charm contributions, respectively.
2018
35th International Symposium on Lattice Field Theory, Lattice 2017
High Energy Physics - Lattice; High Energy Physics - Lattice; High Energy Physics - Phenomenology
04 Pubblicazione in atti di convegno::04c Atto di convegno in rivista
HVP contributions to the muon (g -2) including QED corrections with twisted-mass fermions / Giusti, D.; Lubicz, V.; Martinelli, G.; Sanfilippo, F.; Simula, S.. - In: EPJ WEB OF CONFERENCES. - ISSN 2100-014X. - 175:(2018), p. 06006. (Intervento presentato al convegno 35th International Symposium on Lattice Field Theory, Lattice 2017 tenutosi a Exhibition and Conference Centre in Granada, esp) [10.1051/epjconf/201817506006].
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11573/1322349
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