pith. sign in

arxiv: 2607.00564 · v1 · pith:Z66RZ4A6new · submitted 2026-07-01 · ✦ hep-lat · hep-ph

Isospin-breaking effects in inclusive hadronic τ data for the muon (g-2) from first principles

Pith reviewed 2026-07-02 02:09 UTC · model grok-4.3

classification ✦ hep-lat hep-ph
keywords Lattice QCDIsospin breakingHadronic tau decaysMuon g-2Hadronic vacuum polarizationRadiative correctionsQED effects
0
0 comments X

The pith

Lattice QCD+QED yields a first-principles strategy to compute isospin-breaking corrections in inclusive hadronic tau decays for the muon g-2.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper develops a method to extract isospin-breaking effects directly from lattice simulations that include both QCD and QED, applied to the full inclusive rate rather than exclusive channels. It divides the radiative corrections into three infrared-safe classes that can be handled separately, giving closed-form expressions for the initial-state pieces and a Euclidean-space prescription for the final-state pieces. The approach also supplies a momentum-scheme renormalization rule for each term at linear order in the isospin-breaking parameters. A sympathetic reader would care because the hadronic-vacuum-polarization contribution to the muon anomaly is limited by the precision with which tau data can be converted to the required isospin-symmetric quantities; removing that conversion uncertainty from first principles would tighten the comparison between theory and experiment.

Core claim

The central claim is that isospin-breaking radiative corrections in inclusive hadronic tau decays can be organized into three infrared-safe classes whose individual contributions are computable from Lattice QCD+QED simulations; analytic expressions are provided for the initial-state class, a direct Euclidean-space strategy is proposed for the final-state class, and a momentum-scheme renormalization prescription is given at first order in the breaking parameters, while non-factorizable pieces are isolated as the remaining obstacle to analytic continuation.

What carries the argument

Separation of radiative corrections into three infrared-safe classes, with analytic initial-state expressions and Euclidean final-state strategy, plus momentum-scheme renormalization at linear order in isospin-breaking parameters.

If this is right

  • The three-class separation allows each piece to be renormalized and computed independently without infrared divergences.
  • Initial-state corrections admit closed analytic forms that can be inserted directly into existing lattice correlators.
  • Final-state corrections can be formulated entirely in Euclidean space, avoiding immediate Minkowski continuation.
  • Renormalization of each term at linear order in the isospin-breaking parameters is fixed once a momentum scheme is chosen.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • If the Euclidean strategy for final-state corrections succeeds, the same framework could be applied to other inclusive processes limited by isospin breaking, such as certain rare kaon decays.
  • Success would reduce the theory error on the tau-derived HVP contribution below the current dominant experimental uncertainty on the muon anomaly.
  • The momentum-scheme renormalization rule supplies a concrete matching condition that could be cross-checked against perturbative calculations at short distances.

Load-bearing premise

That the analytic continuation of the non-factorizable contributions from Euclidean to Minkowski space can be controlled well enough to produce results of the needed precision in the inclusive setup.

What would settle it

A lattice calculation in which the continued non-factorizable contributions produce an uncertainty larger than the target precision for the tau-to-pi-pi conversion factor.

read the original abstract

The knowledge of isospin-breaking effects in hadronic $\tau$ decays is required for a high-precision determination of the Hadronic-Vacuum-Polarization contribution to $(g-2)_\mu$ from experimental $\tau$ data. In this work we present a strategy for their calculation in a fully inclusive setup from first-principles Lattice QCD+QED simulations. We separate radiative corrections in three infrared safe classes, which we study individually. We provide analytic expressions for their effects in the initial state and propose a strategy for final-state corrections directly in Euclidean space. We also examine the non-factorizable contributions and highlight the challenges associated with their analytic continuation from Euclidean to Minkowski space. By studying short-distance corrections in the context of momentum schemes, we provide a prescription for the renormalization of the individual terms at first order in the ispospin-breaking parameters.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 2 minor

Summary. The manuscript presents a strategy for computing isospin-breaking effects in inclusive hadronic τ decays from first-principles Lattice QCD+QED simulations. It separates radiative corrections into three infrared-safe classes studied individually, supplies analytic expressions for initial-state corrections, proposes a Euclidean-space treatment for final-state corrections, examines non-factorizable contributions and the associated analytic-continuation challenges from Euclidean to Minkowski space, and provides a renormalization prescription for the individual terms at first order in the isospin-breaking parameters within momentum schemes.

Significance. If successfully implemented, the strategy would enable a fully first-principles determination of the isospin-breaking corrections required to use inclusive τ data for the hadronic vacuum polarization contribution to (g-2)_μ. This is potentially significant because it could reduce model dependence in the τ-based route and improve the overall precision of the Standard-Model prediction. The separation into three infrared-safe classes and the explicit analytic expressions for initial-state effects constitute concrete, reusable advances that future numerical work can build upon.

major comments (1)
  1. [Discussion of non-factorizable contributions] The viability of the fully inclusive setup rests on controlling the analytic continuation of non-factorizable contributions. The manuscript correctly flags the associated challenges but supplies neither a concrete prescription nor a toy-model test demonstrating that these contributions can be continued with controlled errors at the sub-percent level required for (g-2)_μ.
minor comments (2)
  1. The abstract contains the typographical error 'ispospin-breaking' (should read 'isospin-breaking').
  2. [Renormalization prescription] The renormalization prescription in momentum schemes is stated at first order but would be clearer if accompanied by an explicit formula or worked example showing how the individual classes are renormalized.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their positive summary of our manuscript and for recognizing the potential significance of the proposed strategy. We address the major comment below.

read point-by-point responses
  1. Referee: The viability of the fully inclusive setup rests on controlling the analytic continuation of non-factorizable contributions. The manuscript correctly flags the associated challenges but supplies neither a concrete prescription nor a toy-model test demonstrating that these contributions can be continued with controlled errors at the sub-percent level required for (g-2)_μ.

    Authors: We agree that controlling the analytic continuation of the non-factorizable contributions is essential for the viability of a fully inclusive first-principles calculation at the precision needed for (g-2)_μ. Our manuscript explicitly identifies these challenges (see the relevant discussion in the section on non-factorizable terms) precisely because they constitute a non-trivial open problem. The present work is a strategy paper whose scope is to (i) separate the radiative corrections into three infrared-safe classes, (ii) supply analytic expressions for the initial-state corrections, and (iii) outline a Euclidean-space approach for the final-state corrections. Developing a concrete, numerically controllable prescription for the continuation, together with a toy-model validation at the sub-percent level, would require a dedicated follow-up study that lies outside the scope of this manuscript. We therefore do not supply such a prescription or test here. We are happy to add an explicit statement clarifying the intended scope of the paper if the referee considers it useful. revision: no

Circularity Check

0 steps flagged

No significant circularity in proposed first-principles strategy

full rationale

The manuscript presents a methodological strategy for inclusive isospin-breaking corrections in hadronic tau decays using Lattice QCD+QED. It separates radiative corrections into three infrared-safe classes, supplies analytic expressions for initial-state effects, and outlines a Euclidean-space approach for final-state corrections while explicitly flagging analytic-continuation challenges for non-factorizable terms. No load-bearing step reduces by construction to a fitted parameter, self-definition, or self-citation chain; the central claims remain independent methodological proposals rather than predictions forced by the same inputs. This is the expected outcome for a strategy paper whose derivation chain is self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Only the abstract is available, so the ledger is necessarily incomplete and based on standard domain assumptions for lattice calculations; no explicit free parameters, ad-hoc axioms, or new entities are named in the provided text.

axioms (1)
  • domain assumption Lattice QCD+QED simulations can capture the relevant isospin-breaking effects in an inclusive hadronic tau decay setup.
    The entire strategy rests on the validity of lattice methods for this class of observables.

pith-pipeline@v0.9.1-grok · 5700 in / 1174 out tokens · 38271 ms · 2026-07-02T02:09:40.862601+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

160 extracted references · 136 canonical work pages · 55 internal anchors

  1. [1]

    T. Blum, N. Christ, M. Hayakawa, T. Izubuchi, L. Jin, C. Jung et al.,The hadronic light-by-light scattering contribution to the muon anomalous magnetic moment from lattice QCD,Phys. Rev. Lett.124(2020) 132002 [1911.08123]

  2. [2]

    E.-H. Chao, R. J. Hudspith, A. Gérardin, J. R. Green, H. B. Meyer and K. Ottnad,Hadronic light-by-light contribution to(g−2) µ from lattice QCD: a complete calculation,Eur. Phys. J. C81 (2021) 651 [2104.02632]. – 42 –

  3. [3]

    E.-H. Chao, R. J. Hudspith, A. Gérardin, J. R. Green and H. B. Meyer,The charm-quark contribution to light-by-light scattering in the muon(g−2)from lattice QCD,Eur. Phys. J. C82 (2022) 664 [2204.08844]. [4]RBC, UKQCDcollaboration, T. Blum, N. Christ, M. Hayakawa, T. Izubuchi, L. Jin, C. Jung et al.,Hadronic light-by-light contribution to the muon anomaly ...

  4. [4]

    Fodor, A

    Z. Fodor, A. Gérardin, L. Lellouch, K. K. Szabó, B. C. Toth and C. Zimmermann,Hadronic light-by-light scattering contribution to the anomalous magnetic moment of the muon at the physical pion mass,Phys. Rev. D111(2025) 114509 [2411.11719]

  5. [5]

    Dispersion relation for hadronic light-by-light scattering: theoretical foundations

    G. Colangelo, M. Hoferichter, M. Procura and P. Stoffer,Dispersion relation for hadronic light-by-light scattering: theoretical foundations,JHEP09(2015) 074 [1506.01386]

  6. [6]

    Pseudoscalar-pole contribution to the $(g_{\mu}-2)$: a rational approach

    P. Masjuan and P. Sánchez-Puertas,Pseudoscalar-pole contribution to the(gµ −2): a rational approach,Phys. Rev. D95(2017) 054026 [1701.05829]

  7. [7]

    Dispersion relation for hadronic light-by-light scattering: two-pion contributions

    G. Colangelo, M. Hoferichter, M. Procura and P. Stoffer,Dispersion relation for hadronic light-by-light scattering: two-pion contributions,JHEP04(2017) 161 [1702.07347]

  8. [8]

    Dispersion relation for hadronic light-by-light scattering: pion pole

    M. Hoferichter, B.-L. Hoid, B. Kubis, S. Leupold and S. P. Schneider,Dispersion relation for hadronic light-by-light scattering: pion pole,JHEP10(2018) 141 [1808.04823]

  9. [9]

    Eichmann, C

    G. Eichmann, C. S. Fischer, E. Weil and R. Williams,Single pseudoscalar meson pole and pion box contributions to the anomalous magnetic moment of the muon,Phys. Lett. B797(2019) 134855 [1903.10844]

  10. [10]

    Bijnens, N

    J. Bijnens, N. Hermansson-Truedsson and A. Rodríguez-Sánchez,Short-distance constraints for the HLbL contribution to the muon anomalous magnetic moment,Phys. Lett. B798(2019) 134994 [1908.03331]

  11. [11]

    Leutgeb and A

    J. Leutgeb and A. Rebhan,Axial vector transition form factors in holographic QCD and their contribution to the anomalous magnetic moment of the muon,Phys. Rev. D101(2020) 114015 [1912.01596]

  12. [12]

    Cappiello, O

    L. Cappiello, O. Catà, G. D’Ambrosio, D. Greynat and A. Iyer,Axial-vector and pseudoscalar mesons in the hadronic light-by-light contribution to the muon(g−2),Phys. Rev. D102(2020) 016009 [1912.02779]

  13. [13]

    Masjuan, P

    P. Masjuan, P. Roig and P. Sánchez-Puertas,The interplay of transverse degrees of freedom and axial-vector mesons with short-distance constraints ing−2,J. Phys. G49(2022) 015002 [2005.11761]

  14. [14]

    Bijnens, N

    J. Bijnens, N. Hermansson-Truedsson, L. Laub and A. Rodríguez-Sánchez,Short-distance HLbL contributions to the muon anomalous magnetic moment beyond perturbation theory,JHEP10 (2020) 203 [2008.13487]

  15. [15]

    Bijnens, N

    J. Bijnens, N. Hermansson-Truedsson, L. Laub and A. Rodríguez-Sánchez,The two-loop perturbative correction to the(g−2) µ HLbL at short distances,JHEP04(2021) 240 [2101.09169]

  16. [16]

    Danilkin, M

    I. Danilkin, M. Hoferichter and P. Stoffer,A dispersive estimate of scalar contributions to hadronic light-by-light scattering,Phys. Lett. B820(2021) 136502 [2105.01666]

  17. [17]

    Stamen, D

    D. Stamen, D. Hariharan, M. Hoferichter, B. Kubis and P. Stoffer,Kaon electromagnetic form factors in dispersion theory,Eur. Phys. J. C82(2022) 432 [2202.11106]

  18. [18]

    Leutgeb, J

    J. Leutgeb, J. Mager and A. Rebhan,Hadronic light-by-light contribution to the muong−2from holographic QCD with solvedU(1)A problem,Phys. Rev. D107(2023) 054021 [2211.16562]

  19. [19]

    Hoferichter, B

    M. Hoferichter, B. Kubis and M. Zanke,Axial-vector transition form factors ande+e− →f 1π+π−, JHEP08(2023) 209 [2307.14413]. – 43 –

  20. [20]

    Hoferichter, P

    M. Hoferichter, P. Stoffer and M. Zillinger,An optimized basis for hadronic light-by-light scattering, JHEP04(2024) 092 [2402.14060]

  21. [21]

    E. J. Estrada, S. Gonzàlez-Solís, A. Guevara and P. Roig,Improvedπ0,η,η’ transition form factors in resonance chiral theory and theiraHLbL µ contribution,JHEP12(2024) 203 [2409.10503]

  22. [22]

    Lüdtke, M

    J. Lüdtke, M. Procura and P. Stoffer,Dispersion relations for the hadronic VVA correlator,JHEP 04(2025) 130 [2410.11946]

  23. [23]

    Deineka, I

    O. Deineka, I. Danilkin and M. Vanderhaeghen,Dispersive estimate of the a0(980) contribution to (g-2)µ,Phys. Rev. D111(2025) 034009 [2410.12894]

  24. [24]

    Eichmann, C

    G. Eichmann, C. S. Fischer, T. Haeuser and O. Regenfelder,Axial-vector and scalar contributions to hadronic light-by-light scattering,Eur. Phys. J. C85(2025) 445 [2411.05652]

  25. [25]

    Bijnens, N

    J. Bijnens, N. Hermansson-Truedsson and A. Rodríguez-Sánchez,Constraints on the hadronic light-by-light tensor in corner kinematics for the muon g−2,JHEP03(2025) 094 [2411.09578]

  26. [26]

    Hoferichter, P

    M. Hoferichter, P. Stoffer and M. Zillinger,Dispersion relation for hadronic light-by-light scattering: subleading contributions,JHEP02(2025) 121 [2412.00178]

  27. [27]

    S. Holz, M. Hoferichter, B.-L. Hoid and B. Kubis,Dispersion relation for hadronic light-by-light scattering:ηandη ′ poles,JHEP04(2025) 147 [2412.16281]

  28. [28]

    Cappiello, J

    L. Cappiello, J. Leutgeb, J. Mager and A. Rebhan,Tensor meson transition form factors in holographic QCD and the muong−2,JHEP07(2025) 033 [2501.09699]

  29. [29]

    The anomalous magnetic moment of the muon in the Standard Model

    T. Aoyama et al.,The anomalous magnetic moment of the muon in the Standard Model,Phys. Rept.887(2020) 1 [2006.04822]

  30. [30]

    The anomalous magnetic moment of the muon in the Standard Model: an update

    R. Aliberti et al.,The anomalous magnetic moment of the muon in the Standard Model: an update, 2505.21476

  31. [31]

    Bouchiat and L

    C. Bouchiat and L. Michel,La résonance dans la diffusion mésonπ— mésonπet le moment magnétique anormal du mésonµ,J. Phys. Radium22(1961) 121

  32. [32]

    S. J. Brodsky and E. de Rafael,SUGGESTED BOSON - LEPTON PAIR COUPLINGS AND THE ANOMALOUS MAGNETIC MOMENT OF THE MUON,Phys. Rev.168(1968) 1620

  33. [33]

    B. E. Lautrup and E. de Rafael,Calculation of the sixth-order contribution from the fourth-order vacuum polarization to the difference of the anomalous magnetic moments of muon and electron, Phys. Rev.174(1968) 1835

  34. [34]

    Precise measurement of the e+ e- to pi+ pi- (gamma) cross section with the Initial State Radiation method at BABAR

    M. Gourdin and E. de Rafael,Hadronic contributions to the muon g-factor,Nucl. Phys. B10 (1969) 667. [36]BaBarcollaboration, B. Aubert et al.,Precise measurement of the e+ e- —>pi+ pi- (gamma) cross section with the Initial State Radiation method at BABAR,Phys. Rev. Lett.103(2009) 231801 [0908.3589]. [37]BaBarcollaboration, J. P. Lees et al.,Precise measur...

  35. [35]

    Davier, A

    M. Davier, A. Hoecker, A.-M. Lutz, B. Malaescu and Z. Zhang,Tensions ine+e− →π +π−(γ) measurements: the new landscape of data-driven hadronic vacuum polarization predictions for the muong−2,Eur. Phys. J. C84(2024) 721 [2312.02053]. [43]Muong−2collaboration, B. Abi et al.,Measurement of the Positive Muon Anomalous Magnetic Moment to 0.46 ppm,Phys. Rev. Let...

  36. [36]

    A New Approach for Measuring the Muon Anomalous Magnetic Moment and Electric Dipole Moment

    M. Abe et al.,A New Approach for Measuring the Muon Anomalous Magnetic Moment and Electric Dipole Moment,PTEP2019(2019) 053C02 [1901.03047]

  37. [37]

    Improved Determination of the Hadronic Contribution to the Muon (g-2) and to alpha(M_Z**2) Using new Data from Hadronic Tau Decays

    R. Alemany, M. Davier and A. Hocker,Improved determination of the hadronic contribution to the muon (g-2) and to alpha (M(z)) using new data from hadronic tau decays,Eur. Phys. J.C2(1998) 123 [hep-ph/9703220]

  38. [38]

    Isospin Violation and the Magnetic Moment of the Muon

    V. Cirigliano, G. Ecker and H. Neufeld,Isospin violation and the magnetic moment of the muon, Phys. Lett.B513(2001) 361 [hep-ph/0104267]

  39. [39]

    Radiative tau decay and the magnetic moment of the muon

    V. Cirigliano, G. Ecker and H. Neufeld,Radiative tau decay and the magnetic moment of the muon, JHEP08(2002) 002 [hep-ph/0207310]

  40. [40]

    Long-distance radiative corrections to the di-pion tau lepton decay

    F. Flores-Báez, A. Flores-Tlalpa, G. López Castro and G. Toledo,Long-distance radiative corrections to the di-pion tau lepton decay,Phys. Rev. D74(2006) 071301 [hep-ph/0608084]

  41. [41]

    J. A. Miranda and P. Roig,Newτ-based evaluation of the hadronic contribution to the vacuum polarization piece of the muon anomalous magnetic moment,Phys. Rev. D102(2020) 114017 [2007.11019]

  42. [42]

    Confronting Spectral Functions from e+e- Annihilation and tau Decays: Consequences for the Muon Magnetic Moment

    M. Davier, S. Eidelman, A. Hocker and Z. Zhang,Confronting spectral functions from e+ e- annihilation and tau decays: Consequences for the muon magnetic moment,Eur. Phys. J.C27 (2003) 497 [hep-ph/0208177]

  43. [43]

    Model-dependent radiative corrections to tau- -> pi- pi0 nu revisited

    A. Flores-Tlalpa, F. Flores-Báez, G. López Castro and G. Toledo,Model-dependent radiative corrections to tau- —>pi- pi0 nu revisited,Nucl. Phys. B Proc. Suppl.169(2007) 250 [hep-ph/0611226]

  44. [44]

    F. V. Flores-Baéz, G. López Castro and G. Toledo,The Width difference of rho vector mesons, Phys. Rev. D76(2007) 096010 [0708.3256]

  45. [45]

    The Discrepancy Between tau and e+e- Spectral Functions Revisited and the Consequences for the Muon Magnetic Anomaly

    M. Davier, A. Hoecker, G. López Castro, B. Malaescu, X. H. Mo, G. Toledo et al.,The Discrepancy Between tau and e+e- Spectral Functions Revisited and the Consequences for the Muon Magnetic Anomaly,Eur. Phys. J. C66(2010) 127 [0906.5443]

  46. [46]

    López Castro, A

    G. López Castro, A. Miranda and P. Roig,Isospin breaking corrections in 2πproduction in tau decays and e+e- annihilation: Consequences for the muon g-2 and conserved vector current tests, Phys. Rev. D111(2025) 073004 [2411.07696]

  47. [47]

    Comparison of the hadronic vacuum polarization between hadronic $\tau$-decay data and lattice QCD

    N. Allen, D. Boito, M. Golterman, K. Maltman, L. M. Mansur and S. Peris,Comparison of the hadronic vacuum polarization between hadronicτ-decay data and lattice QCD,2605.12205

  48. [48]

    Monnard,Radiative corrections for the two-pion contribution to the hadronic vacuum polarization contribution to the muong−2, Ph.D

    J. Monnard,Radiative corrections for the two-pion contribution to the hadronic vacuum polarization contribution to the muong−2, Ph.D. thesis, Universität Bern, 7, 2021

  49. [49]

    Colangelo, M

    G. Colangelo, M. Cottini, M. Hoferichter and S. Holz,Radiative corrections toτ→ππντ,JHEP02 (2026) 181 [2511.07507]

  50. [50]

    M. Cè, T. Harris, H. B. Meyer, A. Toniato and C. Török,Vacuum correlators at short distances from lattice QCD,JHEP12(2021) 215 [2106.15293]. – 45 –

  51. [51]

    Husung, P

    N. Husung, P. Marquard and R. Sommer,Asymptotic behavior of cutoff effects in Yang–Mills theory and in Wilson’s lattice QCD,Eur. Phys. J. C80(2020) 200 [1912.08498]

  52. [52]

    Husung,Logarithmic corrections to O(a) and O(a2) effects in lattice QCD with Wilson or Ginsparg–Wilson quarks,Eur

    N. Husung,Logarithmic corrections to O(a) and O(a2) effects in lattice QCD with Wilson or Ginsparg–Wilson quarks,Eur. Phys. J. C83(2023) 142 [2206.03536]

  53. [53]

    Sommer, L

    R. Sommer, L. Chimirri and N. Husung,Log-enhanced discretization errors in integrated correlation functions,PoSLA TTICE2022(2023) 358 [2211.15750]

  54. [54]

    M. T. Hansen and A. Patella,Finite-volume effects in(g−2)HVP,LO µ ,Phys. Rev. Lett.123(2019) 172001 [1904.10010]

  55. [55]

    M. T. Hansen and A. Patella,Finite-volume and thermal effects in the leading-HVP contribution to muonic(g−2),JHEP10(2020) 029 [2004.03935]. [65]RBC, UKQCDcollaboration, T. Blum, P. A. Boyle, V. Gülpers, T. Izubuchi, L. Jin, C. Jung et al.,Calculation of the hadronic vacuum polarization contribution to the muon anomalous magnetic moment,Phys. Rev. Lett.121...

  56. [56]

    Electromagnetic and strong isospin-breaking corrections to the muon $g - 2$ from Lattice QCD+QED

    D. Giusti, V. Lubicz, G. Martinelli, F. Sanfilippo and S. Simula,Electromagnetic and strong isospin-breaking corrections to the muong−2from Lattice QCD+QED,Phys. Rev.D99(2019) 114502 [1901.10462]

  57. [57]

    Borsányi et al.,Leading hadronic contribution to the muon magnetic moment from lattice QCD, Nature593(2021) 51 [2002.12347]

    S. Borsányi et al.,Leading hadronic contribution to the muon magnetic moment from lattice QCD, Nature593(2021) 51 [2002.12347]

  58. [58]

    Lehner and A

    C. Lehner and A. S. Meyer,Consistency of hadronic vacuum polarization between lattice QCD and the R-ratio,Phys. Rev. D101(2020) 074515 [2003.04177]. [69]χQCDcollaboration, G. Wang, T. Draper, K.-F. Liu and Y.-B. Yang,Muon g-2 with overlap valence fermions,Phys. Rev. D107(2023) 034513 [2204.01280]

  59. [59]

    Aubin, T

    C. Aubin, T. Blum, M. Golterman and S. Peris,Muon anomalous magnetic moment with staggered fermions: Is the lattice spacing small enough?,Phys. Rev. D106(2022) 054503 [2204.12256]

  60. [60]

    Cè et al.,Window observable for the hadronic vacuum polarization contribution to the muon g−2from lattice QCD,Phys

    M. Cè et al.,Window observable for the hadronic vacuum polarization contribution to the muon g−2from lattice QCD,Phys. Rev. D106(2022) 114502 [2206.06582]. [72]ETMcollaboration, C. Alexandrou et al.,Lattice calculation of the short and intermediate time-distance hadronic vacuum polarization contributions to the muon magnetic moment using twisted-mass ferm...

  61. [61]

    Kuberski, M

    S. Kuberski, M. Cè, G. von Hippel, H. B. Meyer, K. Ottnad, A. Risch et al.,Hadronic vacuum polarization in the muon g−2: the short-distance contribution from lattice QCD,JHEP03(2024) 172 [2401.11895]

  62. [62]

    Hybrid calculation of hadronic vacuum polarization in muon g-2 to 0.48\%

    A. Boccaletti et al.,High precision calculation of the hadronic vacuum polarisation contribution to the muon anomaly,2407.10913

  63. [63]

    Spiegel and C

    S. Spiegel and C. Lehner,High-precision continuum limit study of the HVP short-distance window, Phys. Rev. D111(2025) 114517 [2410.17053]. [77]RBC, UKQCDcollaboration, T. Blum et al.,The long-distance window of the hadronic vacuum polarization for the muon g-2,Phys. Rev. Lett.134(2025) 201901 [2410.20590]

  64. [64]

    Djukanovic, G

    D. Djukanovic, G. von Hippel, S. Kuberski, H. B. Meyer, N. Miller, K. Ottnad et al.,The hadronic vacuum polarization contribution to the muon g−2 at long distances,JHEP04(2025) 098 [2411.07969]. [79]ETMcollaboration, C. Alexandrou et al.,Strange and charm quark contributions to the muon – 46 – anomalous magnetic moment in lattice QCD with twisted-mass fer...

  65. [65]

    Parrino, V

    J. Parrino, V. Biloshytskyi, E.-H. Chao, H. B. Meyer and V. Pascalutsa,Computing the UV-finite electromagnetic corrections to the hadronic vacuum polarization in the muon (g−2) from lattice QCD,JHEP07(2025) 201 [2501.03192]

  66. [66]

    Ray et al.,Calculating the QED correction to the hadronic vacuum polarisation on the lattice, PoSLA TTICE2022(2023) 329 [2212.12031]

    G. Ray et al.,Calculating the QED correction to the hadronic vacuum polarisation on the lattice, PoSLA TTICE2022(2023) 329 [2212.12031]

  67. [67]

    Altherr et al.,Update on the isospin breaking corrections to the HVP with C-periodic boundary conditions,PoSLA TTICE2025(2025) 119 [2502.14845]

    A. Altherr et al.,Update on the isospin breaking corrections to the HVP with C-periodic boundary conditions,PoSLA TTICE2025(2025) 119 [2502.14845]

  68. [68]

    Bruno, V

    M. Bruno, V. Gülpers, N. Hermansson-Truedsson, C. Lehner, J. Parrino and J. T. Tsang,Isospin breaking corrections to the hadronic vacuum polarization with stochastic coordinate sampling, in 42th International Symposium on Lattice Field Theory, 2, 2026,2602.24132

  69. [69]

    Lehner, J

    C. Lehner, J. Parrino and A. Völklein,Long-distance reconstruction of QED corrections to the hadronic vacuum polarization for the muon g-2,2508.21685

  70. [70]

    Luscher,Volume Dependence of the Energy Spectrum in Massive Quantum Field Theories

    M. Luscher,Volume Dependence of the Energy Spectrum in Massive Quantum Field Theories. 1. Stable Particle States,Commun. Math. Phys.104(1986) 177

  71. [71]

    Luscher,Volume Dependence of the Energy Spectrum in Massive Quantum Field Theories

    M. Luscher,Volume Dependence of the Energy Spectrum in Massive Quantum Field Theories. 2. Scattering States,Commun. Math. Phys.105(1986) 153

  72. [72]

    Weak transition matrix elements from finite-volume correlation functions

    L. Lellouch and M. Luscher,Weak transition matrix elements from finite volume correlation functions,Commun. Math. Phys.219(2001) 31 [hep-lat/0003023]

  73. [73]

    H. B. Meyer,Lattice QCD and the Timelike Pion Form Factor,Phys. Rev. Lett.107(2011) 072002 [1105.1892]

  74. [74]

    X. Feng, S. Aoki, S. Hashimoto and T. Kaneko,Timelike pion form factor in lattice QCD,Phys. Rev.D91(2015) 054504 [1412.6319]

  75. [75]

    Erben, J

    F. Erben, J. R. Green, D. Mohler and H. Wittig,Rho resonance, timelike pion form factor, and implications for lattice studies of the hadronic vacuum polarization,Phys. Rev. D101(2020) 054504 [1910.01083]

  76. [76]

    The $I=1$ pion-pion scattering amplitude and timelike pion form factor from $N_{\rm f} = 2+1$ lattice QCD

    C. Andersen, J. Bulava, B. Hörz and C. Morningstar,TheI= 1pion-pion scattering amplitude and timelike pion form factor fromNf = 2 + 1lattice QCD,Nucl. Phys. B939(2019) 145 [1808.05007]

  77. [77]

    M. T. Hansen, H. B. Meyer and D. Robaina,From deep inelastic scattering to heavy-flavor semileptonic decays: Total rates into multihadron final states from lattice qcd,Physical Review D96 (2017) . – 47 –

  78. [78]

    Bulava and M

    J. Bulava and M. T. Hansen,Scattering amplitudes from finite-volume spectral functions,Phys. Rev. D100(2019) 034521 [1903.11735]

  79. [79]

    Hansen, A

    M. Hansen, A. Lupo and N. Tantalo,Extraction of spectral densities from lattice correlators, Physical Review D99(2019)

  80. [80]

    Bailas, S

    G. Bailas, S. Hashimoto and T. Ishikawa,Reconstruction of smeared spectral function from Euclidean correlation functions,PTEP2020(2020) 043B07 [2001.11779]

Showing first 80 references.