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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

The hadronic vacuum polarisation contributions to the anomalous magnetic moment of the muon, $a_{\mu}^{\rm had, VP}$ are evaluated dispersively via a combination of experimentally measured $e^+e^-\rightarrow {\rm hadrons}$ cross section…

High Energy Physics - Experiment · Physics 2019-03-26 Alexander Keshavarzi

Using dispersion relations, we derive the complete virtual QED contributions to Bhabha scattering due to vacuum polarization effects in photon propagation. We apply our result to hadronic corrections and to heavy lepton and top quark loop…

High Energy Physics - Phenomenology · Physics 2008-11-26 Stefano Actis , Michal Czakon , Janusz Gluza , Tord Riemann

We discuss the interplay between two first-principles calculations of QCD at high density: perturbative results in the weak-coupling regime and the recent lattice-QCD result at finite isospin density. By comparing these two results, we…

High Energy Physics - Phenomenology · Physics 2024-09-09 Yuki Fujimoto

In this work we propose a method for including strong isospin breaking in twisted mass lattice calculations, while preserving flavor identification. We utilize a partially quenched construction in which the sea quarks are given by the…

High Energy Physics - Lattice · Physics 2009-04-18 Andre Walker-Loud

A QCD analysis of the world data on polarized deep inelastic scattering is presented in leading and next-to-leading order. New parameterizations are derived for the quark and gluon distributions for the kinematic range $x \epsilon…

High Energy Physics - Phenomenology · Physics 2016-09-06 J. Blümlein , H. Böttcher

The BNL and FNAL measurements of the anomalous magnetic moment of the muon disagree with the Standard Model (SM) prediction by more than $4\sigma$. The hadronic vacuum polarization (HVP) contributions are the dominant source of uncertainty…

High Energy Physics - Phenomenology · Physics 2023-10-19 Andrew Fowlie , Qiao Li

We outline a strategy to efficiently include the electromagnetic interactions of the sea quarks in QCD+QED. When computing iso-spin breaking corrections to hadronic quantities at leading order in the electromagnetic coupling, the sea-quark…

High Energy Physics - Lattice · Physics 2026-05-04 Tim Harris , Vera Gülpers , Antonin Portelli , James Richings

We present a lattice computation of the isospin-breaking corrections to pseudoscalar meson masses using the gauge configurations produced by the European Twisted Mass collaboration with $N_f = 2 + 1 + 1$ dynamical quarks at three values of…

High Energy Physics - Lattice · Physics 2017-06-21 D. Giusti , V. Lubicz , G. Martinelli , F. Sanfilippo , S. Simula , N. Tantalo , C. Tarantino

Isospin symmetry breaking in the quark condensates, $< \bar dd> \not= < \bar uu>$, is a fundamental parameter in both the QCD sum rule studies and the chiral perturbation theory. In this article, we apply the QCD sum rule method to treat…

High Energy Physics - Phenomenology · Physics 2007-05-23 W-Y. P. Hwang , Kwei-Chou Yang

A highly physical model of the subtracted $I=1$ vector polarization, obtained using a dispersive representation with precise hadronic $\tau$ decay data as input, is used to investigate systematic issues in the lattice evaluation of the…

High Energy Physics - Lattice · Physics 2014-10-28 Maarten Golterman , Kim Maltman , Santiago Peris

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

We discuss techniques and results for the extraction of the nucleon's spin-dependent parton distributions and their uncertainties from data for polarized deep-inelastic lepton-nucleon and proton-proton scattering by means of a global QCD…

High Energy Physics - Phenomenology · Physics 2009-09-01 Daniel de Florian , Rodolfo Sassot , Marco Stratmann , Werner Vogelsang

The anomalous magnetic moment of the muon ($\,a_{\mu}\,$) provides a stringent test of the quantum nature of the Standard Model (SM) and its extensions. To probe beyond the SM physics, one needs to be able to subtract the SM contributions,…

High Energy Physics - Phenomenology · Physics 2025-08-25 Kaustubh Agashe , Abhishek Banerjee , Minuyan Jiang , Shmuel Nussinov , Kushan Panchal , Srijit Paul , Gilad Perez , Yotam Soreq

The long-distance contribution of QED corrections to the hadronic vacuum polarization is particularly challenging to compute in lattice QCD+QED. Currently, it is one of the limiting factors towards matching the precision of the recent…

High Energy Physics - Lattice · Physics 2025-09-01 Christoph Lehner , Julian Parrino , Andreas Völklein

We discuss the calculation of the leading hadronic vacuum polarization in lattice QCD. Exploiting the excellent quality of the compiled experimental data for the e^+e^- --> hadrons cross-section, we predict the outcome of large-volume…

High Energy Physics - Lattice · Physics 2015-05-28 David Bernecker , Harvey B. Meyer

Hadronic vacuum polarization at low virtualities limits the precision of experimental tests of the standard model via important physical observables. Here we compute that effect in two-flavor chiral perturbation theory to three loops. Among…

High Energy Physics - Phenomenology · Physics 2026-03-02 Laurent Lellouch , Alessandro Lupo , Mattias Sjö , Kálmán Szabo , Pierre Vanhove

The hadronic contribution to the muon anomalous magnetic moment $a_\mu=(g_\mu-2)/2$ has to be determined at the per-mille level for the Standard Model prediction to match the expected final uncertainty of the ongoing E989 experiment. That…

High Energy Physics - Lattice · Physics 2021-01-13 Leonardo Giusti , Mattia Dalla Brida , Tim Harris , Michele Pepe

After a brief self-contained introduction to the muon anomalous magnetic moment, (g-2), we review the status of lattice calculations of the hadronic vacuum polarization contribution and present first results from lattice QCD for the…

High Energy Physics - Lattice · Physics 2013-01-15 T. Blum , M. Hayakawa , T. Izubuchi

We demonstrate that the dispersive computation of the threshold enhancements to heavy quark vacuum polarizations is unstable. Because of the slow convergence of the dispersion relations the result critically depends on the intermediate…

High Energy Physics - Phenomenology · Physics 2010-11-01 M. C. Gonzalez-Garcia , F. Halzen , R. A. Vázquez