<p>We compute the isospin-violating part <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27449_Article_IEq1.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="51" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>a</mi> <mi>μ</mi> <mrow> <mi>HVP</mi> <mo>,</mo> <mn>38</mn> </mrow> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {a}_{\mu}^{\textrm{HVP},38} \)</EquationSource> </InlineEquation> of the hadronic-vacuum-polarization (HVP) contribution to the muon (<i>g</i> − 2) in lattice QCD at the SU(3)<sub>f</sub>-symmetric point where <i>M</i><sub><i>π</i></sub> = <i>M</i><sub><i>K</i></sub> ≃ 416 MeV. All diagrams involving internal photons are evaluated in coordinate space, employing a Pauli-Villars-regulated photon propagator with a cutoff scale Λ well below the lattice cutoff. The counterterm (<i>m</i><sub><i>u</i></sub> – <i>m</i><sub><i>d</i></sub>), whose Λ dependence is consistent with the expected logarithmic behaviour, is calibrated using the experimental kaon mass splitting as input. The bare electromagnetic contribution at fixed Λ is compared to a phenomenological estimate based on the kaon-loop and pseudoscalar-pole contributions to the forward light-by-light amplitude. An extension of these calculations to physical pion and kaon masses appears promising.</p>

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Isospin-violating vacuum polarization in the muon (g − 2) with SU(3) flavour symmetry from lattice QCD

  • Dominik Erb,
  • Antoine Gérardin,
  • Harvey B. Meyer,
  • Julian Parrino,
  • Volodymyr Biloshytskyi,
  • Vladimir Pascalutsa

摘要

We compute the isospin-violating part a μ HVP , 38 \( {a}_{\mu}^{\textrm{HVP},38} \) of the hadronic-vacuum-polarization (HVP) contribution to the muon (g − 2) in lattice QCD at the SU(3)f-symmetric point where Mπ = MK ≃ 416 MeV. All diagrams involving internal photons are evaluated in coordinate space, employing a Pauli-Villars-regulated photon propagator with a cutoff scale Λ well below the lattice cutoff. The counterterm (mumd), whose Λ dependence is consistent with the expected logarithmic behaviour, is calibrated using the experimental kaon mass splitting as input. The bare electromagnetic contribution at fixed Λ is compared to a phenomenological estimate based on the kaon-loop and pseudoscalar-pole contributions to the forward light-by-light amplitude. An extension of these calculations to physical pion and kaon masses appears promising.