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We calculate the contribution to the muon anomalous magnetic moment hadronic vacuum polarization from {the} connected diagrams of up and down quarks, omitting electromagnetism. We employ QCD gauge-field configurations with dynamical $u$,…

The QCD coupling appears in the perturbative expansion of the current-current two-point (vacuum polarization) function. Any lattice calculation of vacuum polarization is plagued by several competing non-perturbative effects at small momenta…

High Energy Physics - Lattice · Physics 2015-10-19 Renwick J. Hudspith , Randy Lewis , Kim Maltman , Eigo Shintani

We compute the vacuum polarisation on the lattice in quenched QCD using non-perturbatively improved Wilson fermions. Above Q^2 of about 2 GeV^2 the results are very close to the predictions of perturbative QCD. Below this scale we see signs…

High Energy Physics - Lattice · Physics 2008-11-26 M. Göckeler , R. Horsley , W. Kürzinger , D. Pleiter , P. E. L. Rakow , G. Schierholz

Progress in the improvement program in nonrelativistic lattice QCD is outlined. The leading radiative corrections to the heavy-quark mass renormalization, energy shift, and two important kinetic coupling coefficients are presented. The…

High Energy Physics - Lattice · Physics 2010-11-01 Colin J. Morningstar

The anomalous magnetic moment of muon, $g-2$, is a very precisely measured quantity. However, the current measurement disagrees with standard model by about 3 standard deviations. Hadronic vacuum polarization and hadronic light by light are…

High Energy Physics - Lattice · Physics 2015-09-29 Luchang Jin , Thomas Blum , Norman Christ , Masashi Hayakawa , Taku Izubuchi , Christoph Lehner

The electron and muon anomalous magnetic moments (AMM) are measured in experiments and studied in the Standard Model (SM) with the highest precision accessible in particle physics. The comparison of the measured quantity with the SM…

High Energy Physics - Phenomenology · Physics 2015-06-19 A. E. Dorokhov , A. E. Radzhabov , A. S. Zhevlakov

Isospin symmetry is explicitly broken in the Standard Model by the non-zero differences of mass and electric charge between the up and down quarks. Both of these corrections are expected to have a comparable size of the order of one percent…

High Energy Physics - Lattice · Physics 2013-09-11 Antonin Portelli

We present the current Standard Model (SM) prediction for the muon anomalous magnetic moment, $a_\mu$, updating the first White Paper (WP20) [1]. The pure QED and electroweak contributions have been further consolidated, while hadronic…

High Energy Physics - Phenomenology · Physics 2025-09-12 R. Aliberti , T. Aoyama , E. Balzani , A. Bashir , G. Benton , J. Bijnens , V. Biloshytskyi , T. Blum , D. Boito , M. Bruno , E. Budassi , S. Burri , L. Cappiello , C. M. Carloni Calame , M. Cè , V. Cirigliano , D. A. Clarke , G. Colangelo , L. Cotrozzi , M. Cottini , I. Danilkin , M. Davier , M. Della Morte , A. Denig , C. DeTar , V. Druzhinin , G. Eichmann , A. X. El-Khadra , E. Estrada , X. Feng , C. S. Fischer , R. Frezzotti , G. Gagliardi , A. Gérardin , M. Ghilardi , D. Giusti , M. Golterman , S. Gonzàlez-Solís , S. Gottlieb , R. Gruber , A. Guevara , V. Gülpers , A. Gurgone , F. Hagelstein , M. Hayakawa , N. Hermansson-Truedsson , A. Hoecker , M. Hoferichter , B. -L. Hoid , S. Holz , R. J. Hudspith , F. Ignatov , L. Jin , N. Kalntis , G. Kanwar , A. Keshavarzi , J. Komijani , J. Koponen , S. Kuberski , B. Kubis , A. Kupich , A. Kupść , S. Lahert , S. Laporta , C. Lehner , M. Lellmann , L. Lellouch , T. Leplumey , J. Leutgeb , T. Lin , Q. Liu , I. Logashenko , C. Y. London , G. López Castro , J. Lüdtke , A. Lusiani , A. Lutz , J. Mager , B. Malaescu , K. Maltman , M. K. Marinković , J. Márquez , P. Masjuan , H. B. Meyer , T. Mibe , N. Miller , A. Miramontes , A. Miranda , G. Montagna , S. E. Müller , E. T. Neil , A. V. Nesterenko , O. Nicrosini , M. Nio , D. Nomura , J. Paltrinieri , L. Parato , J. Parrino , V. Pascalutsa , M. Passera , S. Peris , P. Petit Rosàs , F. Piccinini , R. N. Pilato , L. Polat , A. Portelli , D. Portillo-Sánchez , M. Procura , L. Punzi , K. Raya , A. Rebhan , C. F. Redmer , B. L. Roberts , A. Rodríguez-Sánchez , P. Roig , J. Ruiz de Elvira , P. Sánchez-Puertas , A. Signer , J. W. Sitison , D. Stamen , D. Stöckinger , H. Stöckinger-Kim , P. Stoffer , Y. Sue , P. Tavella , T. Teubner , J. -N. Toelstede , G. Toledo , W. J. Torres Bobadilla , J. T. Tsang , F. P. Ucci , Y. Ulrich , R. S. Van de Water , G. Venanzoni , S. Volkov , G. von Hippel , G. Wang , U. Wenger , H. Wittig , A. Wright , E. Zaid , M. Zanke , Z. Zhang , M. Zillinger , C. Alexandrou , A. Altherr , M. Anderson , C. Aubin , S. Bacchio , P. Beltrame , A. Beltran , P. Boyle , I. Campos Plasencia , I. Caprini , B. Chakraborty , G. Chanturia , A. Crivellin , A. Czarnecki , L. -Y. Dai , T. Dave , L. Del Debbio , K. Demory , D. Djukanovic , T. Draper , A. Driutti , M. Endo , F. Erben , K. Ferraby , J. Finkenrath , L. Flower , A. Francis , E. Gámiz , J. Gogniat , A. V. Grebe , S. Gündogdu , M. T. Hansen , S. Hashimoto , H. Hayashii , D. W. Hertzog , L. A. Heuser , L. Hostetler , X. T. Hou , G. S. Huang , T. Iijima , K. Inami , A. Jüttner , R. Kitano , M. Knecht , S. Kollatzsch , A. S. Kronfeld , T. Lenz , G. Levati , Q. M. Li , Y. P. Liao , J. Libby , K. F. Liu , V. Lubicz , M. T. Lynch , A. T. Lytle , J. L. Ma , K. Miura , K. Möhling , J. Muskalla , F. Noël , K. Ottnad , P. Paradisi , C. T. Peterson , A. Pich , S. Pitelis , S. Plura , A. Price , D. Radic , A. Radzhabov , A. Risch , S. Romiti , S. Sahoo , F. Sannino , H. Schäfer , Y. Schelhaas , S. I. Serednyakov , O. Shekhovtsova , J. N. Simone , S. Simula , E. P. Solodov , F. M. Stokes , M. Vanderhaeghen , A. Vaquero , N. Vestergaard , W. P. Wang , Z. Wąs , K. Yamashita , Y. B. Yang , T. Yoshioka , C. Z. Yuan , A. S. Zhevlakov

The short-distance behaviour of the hadronic light-by-light (HLbL) contribution to $(g-2)_{\mu}$ has recently been studied by means of an operator product expansion in a background electromagnetic field. The leading term in this expansion…

High Energy Physics - Phenomenology · Physics 2021-05-12 Johan Bijnens , Nils Hermansson-Truedsson , Laetitia Laub , Antonio Rodríguez-Sánchez

We present a calculation of the hadronic vacuum polarization contribution to the muon anomalous magnetic moment, $a_\mu^{\mathrm hvp}$, in lattice QCD employing dynamical up and down quarks. We focus on controlling the infrared regime of…

High Energy Physics - Lattice · Physics 2017-10-11 M. Della Morte , A. Francis , V. Gülpers , G. Herdoíza , G. von Hippel , H. Horch , B. Jäger , H. B. Meyer , A. Nyffeler , H. Wittig

The leading-order hadronic contribution to the muon anomalous magentic moment, $a_\mu^{\rm LO,HVP}$, can be expressed as an integral over Euclidean $Q^2$ of the vacuum polarization function. We point out that a simple trapezoid-rule…

High Energy Physics - Lattice · Physics 2014-10-31 Maarten Golterman , Kim Maltman , Santiago Peris

Chiral dynamics makes definitive predictions for the electromagnetic polarizabilities of hadrons near the chiral limit; but, agreement with experiment is tenuous in some cases. We provide an overview of lattice QCD methods to compute the…

High Energy Physics - Lattice · Physics 2013-01-22 B. C. Tiburzi

We study the four most significant high precision observables of QED ---the anomalous electron and muon magnetic moments, the hydrogen Lamb shift and muonium hyperfine splitting--- in the context of SU(2) x U(1) gauge-invariant effective…

High Energy Physics - Phenomenology · Physics 2011-09-13 Rafel Escribano , Eduard Masso

We report our (HPQCD) progress on the calculation of the Hadronic Vacuum Polarisation contribution to the anomalous magnetic moment of muon. In this article we discuss the calculations for the light (up/down) quark connected contribution…

High Energy Physics - Lattice · Physics 2015-11-19 Bipasha Chakraborty , Christine Davies , Pedro Gonçalves de Oliveira , Jonna Koponen , G. Peter Lepage

I provide updates for the theoretical predictions of the muon and electron anomalous magnetic moments, for the shift in the fine structure constant $\alpha(M_Z)$ and for the weak mixing parameter $\sin^2 \Theta_W(M_Z)$. Phenomenological…

High Energy Physics - Phenomenology · Physics 2017-11-17 Fred Jegerlehner

Electroweak, QCD, and QED radiative corrections to the nucleon low-energy coupling constants $g_V$ and $g_A$ are enhanced by large perturbative logarithms between the electroweak and hadronic scale, as well as between the hadronic scale and…

High Energy Physics - Phenomenology · Physics 2026-04-10 Oleksandr Tomalak , Yi-Bo Yang

We discuss a recently introduced strategy to study non-perturbatively thermal QCD up to temperatures of the order of the electro-weak scale, combining step scaling techniques and shifted boundary conditions. The former allow to renormalize…

High Energy Physics - Lattice · Physics 2024-11-22 Leonardo Giusti , Davide Laudicina , Matteo Bresciani , Mattia Dalla Brida , Tim Harris , Michele Pepe , Pietro Rescigno

The hadronic contributions to the muon anomalous magnetic moment and to the shift of the electromagnetic fine structure constant at the scale of Z boson mass are evaluated within dispersively improved perturbation theory (DPT). The latter…

High Energy Physics - Phenomenology · Physics 2017-10-24 A. V. Nesterenko

We measure the hadronic contribution to the vacuum polarisation tensor, and use it to estimate the hadronic contribution to (g-2)_mu, the muon anomalous magnetic moment.

High Energy Physics - Lattice · Physics 2008-11-26 M. Göckeler , R. Horsley , W. Kürzinger , D. Pleiter , P. E. L. Rakow , G. Schierholz

We consider the process of muon-electron elastic scattering, which has been proposed as an ideal framework to measure the running of the electromagnetic coupling constant at space-like momenta and determine the leading-order hadronic…

High Energy Physics - Phenomenology · Physics 2019-03-05 Massimo Alacevich , Carlo M. Carloni Calame , Mauro Chiesa , Guido Montagna , Oreste Nicrosini , Fulvio Piccinini
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