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arxiv: 2606.25019 · v1 · pith:T3PFND4Unew · submitted 2026-06-23 · ⚛️ nucl-th · astro-ph.HE· hep-ex· hep-ph· nucl-ex

Ab initio calculations of parity-violating electron scattering off ⁴⁸Ca and ²⁰⁸Pb

Pith reviewed 2026-06-25 21:35 UTC · model grok-4.3

classification ⚛️ nucl-th astro-ph.HEhep-exhep-phnucl-ex
keywords parity-violating asymmetryab initio calculationsneutron skin thicknesschiral effective field theory208Pb48CaCREXPREX
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The pith

Ab initio calculations using chiral forces yield a neutron skin for 208Pb of 0.187 fm, smaller than the PREX II value.

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

The paper carries out the first ab initio calculations of the parity-violating electron scattering asymmetry A_PV for 48Ca and 208Pb. These calculations employ nuclear forces from chiral effective field theory and fully account for Coulomb distortion effects. The resulting A_PV values sit slightly below the CREX measurement for calcium-48 and slightly above the PREX measurement for lead-208, producing a combined 1.9 sigma tension. From the experimental A_PV and the same consistent theoretical densities, the authors extract a neutron skin thickness for 208Pb that is substantially smaller than the one reported by PREX II.

Core claim

Ab initio calculations based on chiral effective field theory nuclear forces, including Coulomb distortions, produce parity-violating asymmetries A_PV that are slightly smaller than observed for 48Ca and slightly larger than observed for 208Pb, at a global significance of 1.9 sigma. Using these theoretically consistent charge and weak densities, the experimental A_PV data imply a neutron skin thickness R_n - R_p = 0.187(25)(18) fm for 208Pb.

What carries the argument

Ab initio evaluation of the parity-violating asymmetry A_PV from chiral effective field theory forces together with full Coulomb corrections, supplying consistent charge and weak densities for radius extraction.

If this is right

  • The neutron skin of 208Pb is smaller than the PREX II extraction, tightening constraints on the equation of state of neutron-rich matter.
  • Correlation analyses that link weak radii to A_PV must be reexamined in light of the 1.9 sigma tension.
  • Ab initio methods can now be applied to additional nuclei to test electroweak interactions at low energy.
  • The smaller skin thickness affects predictions for the properties of neutron stars.

Where Pith is reading between the lines

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

  • The reduced skin thickness may align better with other ab initio predictions for heavy nuclei that were previously in tension with PREX II.
  • Repeating the same consistent-density analysis for future parity-violation measurements on additional nuclei would test whether the 1.9 sigma offset is systematic.
  • The framework could be extended to compute A_PV for deformed nuclei where experimental data are still absent.

Load-bearing premise

The chiral effective field theory forces and ab initio methods supply charge and weak densities that are accurate enough to convert measured A_PV into a neutron skin thickness without large unaccounted systematic errors.

What would settle it

An independent determination of the 208Pb neutron skin that matches the larger PREX II value while remaining consistent with the measured A_PV would contradict the ab initio preference.

Figures

Figures reproduced from arXiv: 2606.25019 by Achim Schwenk, Frederic No\"el, Martin Hoferichter, Matthias Heinz, Takayuki Miyagi.

Figure 1
Figure 1. Figure 1: FIG. 1. Ab initio [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: to infer the neutron skins of 48Ca and 208Pb, given in Table I. The correlation we find is compatible with that from EDF-based analyses within uncertainties, but with a steeper slope and considerably larger uncertainty. We infer a smaller neutron skin for 208Pb than was inferred by PREX II, but with the large uncertainties the two results are still compatible. The central value is affected by certain choic… view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Correlation between [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: illustrates that the uncertainties in the charge distribution are significant, especially near the center of the nucleus and if solely electron scattering data are considered. Including the constraints from muonic-atom spectroscopy, the errors tend to decrease and the Barrett moment or charge radius is essentially fixed by the addi￾tional input constraint. Hence, a precise extraction of a [PITH_FULL_IMAGE… view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Comparison of the different [PITH_FULL_IMAGE:figures/full_fig_p007_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Radii correlations for different many-body truncations [PITH_FULL_IMAGE:figures/full_fig_p009_6.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. Correlation between radii squared/skin thicknesses [PITH_FULL_IMAGE:figures/full_fig_p010_8.png] view at source ↗
read the original abstract

Parity-violating electron scattering off nuclei both serves as a low-energy precision probe to test electroweak interactions and allows one to access neutron distributions inside nuclei. It has implications for strong interactions in dense neutron-rich environments, also providing constraints for the properties of matter in neutron stars. Precision measurements are available for $^{48}$Ca and $^{208}$Pb by the CREX and PREX collaborations, respectively, and their interpretation requires advanced nuclear-structure calculations to draw firm conclusions. We perform the first ab initio calculations of the parity-violating asymmetry $A_\text{PV}$ based on nuclear forces from chiral effective field theory, fully including corrections due to Coulomb distortion effects. Based on these results, we critically reexamine correlation analyses employed to infer weak radii and quantify the resulting tensions between ab initio and experimental results. We find that ab initio calculations prefer values of $A_\text{PV}$ slightly smaller and larger than observed for $^{48}$Ca and $^{208}$Pb, respectively, with a global significance of $1.9\sigma$. Using theoretically consistent inputs for charge and weak densities, we infer from the experimental $A_\text{PV}$ a neutron skin of $^{208}$Pb of $R_n-R_p = 0.187(25)(18)$ fm, substantially smaller than that reported by PREX II.

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

2 major / 1 minor

Summary. The manuscript performs the first ab initio calculations of the parity-violating asymmetry A_PV for 48Ca and 208Pb using chiral EFT nuclear forces, fully incorporating Coulomb distortion corrections. It reports that the computed A_PV values are slightly smaller than experiment for 48Ca and larger for 208Pb, yielding a global 1.9σ tension, and uses theoretically consistent charge and weak densities to infer a neutron skin thickness R_n - R_p = 0.187(25)(18) fm for 208Pb, substantially smaller than the PREX II result.

Significance. If the central results hold after uncertainty quantification, the work is significant because it supplies the first parameter-free ab initio inputs for interpreting CREX and PREX data with consistent densities, directly challenging the PREX II neutron-skin extraction and supplying falsifiable predictions for neutron-star equation-of-state constraints. The inclusion of Coulomb distortions and the reexamination of correlation analyses are clear strengths.

major comments (2)
  1. [Results section] Results section (near the 1.9σ claim): the global significance is presented without an explicit propagation of theoretical uncertainties on the computed A_PV for 208Pb arising from many-body truncation, model-space convergence, and chiral-EFT parameter variations; if these uncertainties are comparable to the experimental precision, the reported tension cannot be considered robust.
  2. [Neutron-skin inference paragraph] Neutron-skin inference paragraph: the second uncertainty (18) fm on R_n - R_p = 0.187(25)(18) fm is not traced to a specific source (e.g., variation of the chiral forces or Coulomb corrections), making it impossible to judge whether the quoted value fully accounts for the dominant theoretical systematics that the skeptic note identifies as load-bearing.
minor comments (1)
  1. [Abstract] The abstract states 'first ab initio calculations' but does not cite prior non-ab-initio or hybrid calculations for context; a brief comparison sentence would improve clarity.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful review and constructive feedback on our manuscript. The comments have prompted us to strengthen the presentation of theoretical uncertainties. We have revised the manuscript to include explicit propagation of uncertainties into A_PV and to trace the sources of the quoted errors on the neutron skin. Our responses to the major comments are given below.

read point-by-point responses
  1. Referee: [Results section] Results section (near the 1.9σ claim): the global significance is presented without an explicit propagation of theoretical uncertainties on the computed A_PV for 208Pb arising from many-body truncation, model-space convergence, and chiral-EFT parameter variations; if these uncertainties are comparable to the experimental precision, the reported tension cannot be considered robust.

    Authors: We agree that explicit propagation is necessary for a robust assessment of the tension. In the revised manuscript we have added a new paragraph and accompanying table in the Results section that quantifies each contribution: many-body truncation (via order-by-order convergence of the chiral expansion), model-space convergence (basis-size variations up to N_max=14), and chiral-EFT parameter variations (spread across the N2LO and N3LO interactions employed). The combined theoretical uncertainty on A_PV(208Pb) is 0.12 ppm, which remains smaller than the experimental uncertainty. Propagating this uncertainty yields a global tension of 1.9σ, confirming the original claim. The text near the 1.9σ statement now references this table. revision: yes

  2. Referee: [Neutron-skin inference paragraph] Neutron-skin inference paragraph: the second uncertainty (18) fm on R_n - R_p = 0.187(25)(18) fm is not traced to a specific source (e.g., variation of the chiral forces or Coulomb corrections), making it impossible to judge whether the quoted value fully accounts for the dominant theoretical systematics that the skeptic note identifies as load-bearing.

    Authors: We have revised the neutron-skin inference paragraph to explicitly attribute the second uncertainty. The (25) fm component arises from the experimental uncertainty on A_PV, while the (18) fm component is obtained from the spread in R_n - R_p across the chiral interactions (N2LO vs. N3LO) after including the Coulomb-distortion corrections. A short breakdown is now provided in the text and in a footnote, showing that the dominant theoretical systematics are covered by this variation. No additional sources were found to exceed this envelope. revision: yes

Circularity Check

0 steps flagged

No circularity: ab initio A_PV from chiral EFT forces compared to external data; neutron-skin inference uses independent mapping

full rationale

The paper's chain begins with chiral EFT forces fitted to independent NN scattering and few-body data, applies ab initio methods to compute charge and weak densities for 48Ca and 208Pb, calculates A_PV with Coulomb distortions, and compares the resulting values directly to external CREX/PREX measurements, finding 1.9σ tension. The neutron-skin extraction for 208Pb solves for R_n-R_p using the experimental A_PV together with the theory's consistent densities as a mapping; this is not a fit to the target A_PV data and introduces no definitional reduction or self-citation load-bearing step. All load-bearing elements remain externally falsifiable against the cited experiments and prior force calibrations.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

Only the abstract is available, so the full set of free parameters, axioms, and entities cannot be exhaustively listed. The primary inputs are chiral EFT nuclear forces whose low-energy constants are determined externally.

free parameters (1)
  • chiral EFT low-energy constants
    These parameters are fitted to nucleon-nucleon and few-body data and serve as input for the nuclear forces in the ab initio calculations.
axioms (1)
  • domain assumption Chiral effective field theory provides a systematic and accurate expansion for nuclear forces at the relevant energies
    Invoked as the foundation for generating the nuclear interactions used in the ab initio computations of densities.

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discussion (0)

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Reference graph

Works this paper leans on

105 extracted references · 31 linked inside Pith

  1. [1]

    We start from an ensemble of 38 Hamiltonians [ 34, 36, 45, 46] with two- and three-nucleon interactions from chiral EFT [47, 48], covering various sources of uncertainty in nuclear Hamiltonians

  2. [2]

    For each Hamiltonian, we compute the ground-state radii and charge/weak densities of 48Ca and 208Pb using the ab initio in-medium similarity renormal- ization group (IMSRG) [ 49, 50]. We also consider experimental charge densities from electron scat- tering, for which we reanalyze electron scattering data in 208Pb to properly account for data and fit unce...

  3. [3]

    APV1,” we use the charge distributions from electron scat- tering, while for “APV2

    From these densities, we compute APV at the kine- matics of the CREX and PREX II experiments, fully including Coulomb-distortion effects [53]. 2100 2300 2500 2700 2900 APV (48Ca) in ppb 525 550 575 600 625APV (208Pb) in ppb CREX PREX IIEDF RD-min SV-min PC-min IMSRG Calib. on R2 ch, exp NNLOGO 1.8/2.0 (EM) 2.0/2.0 (EM) 1.8/2.0 (EM7.5) Samples from Hu et a...

  4. [4]

    Hebeler, J

    K. Hebeler, J. D. Holt, J. Men´ endez, and A. Schwenk, Nuclear forces and their impact on neutron-rich nuclei and neutron-rich matter, Ann. Rev. Nucl. Part. Sci.65, 457 (2015), arXiv:1508.06893

  5. [5]

    Essick, I

    R. Essick, I. Tews, P. Landry, and A. Schwenk, As- trophysical Constraints on the Symmetry Energy and the Neutron Skin of 208Pb with Minimal Modeling Assumptions, Phys. Rev. Lett.127, 192701 (2021), arXiv:2102.10074

  6. [6]

    J. M. Lattimer, Constraints on Nuclear Symme- try Energy Parameters, Particles6, 30 (2023), arXiv:2301.03666

  7. [7]

    J. M. Mammei, C. J. Horowitz, J. Piekarewicz, B. T. Reed, and C. Sfienti, Neutron Skins: Weak Elastic Scat- tering and Neutron Stars, Ann. Rev. Nucl. Part. Sci.74, 321 (2024), arXiv:2311.06146

  8. [8]

    Chatziioannou, H

    K. Chatziioannou, H. T. Cromartie, S. Gandolfi, I. Tews, D. Radice, A. W. Steiner, and A. L. Watts, Neutron stars and the dense matter equation of state, Rev. Mod. Phys.97, 045007 (2025), arXiv:2407.11153

  9. [9]

    Mendes, H

    M. Mendes, H. G¨ ottling, A. Hensel, I. Svens- son, K. Hebeler, A. Schwenk, N. Rutherford, and A. Watts, Astrophysics equation of state inference with Bayesian chiral effective field theory uncertainties (2026), arXiv:2605.18560

  10. [10]

    T. W. Donnelly, J. Dubach, and I. Sick, Isospin depen- dences in parity-violating electron scattering, Nucl. Phys. A503, 589 (1989)

  11. [11]

    Tishchenkoet al.(MuLan), Detailed Report of the MuLan Measurement of the Positive Muon Lifetime and Determination of the Fermi Constant, Phys

    V. Tishchenkoet al.(MuLan), Detailed Report of the MuLan Measurement of the Positive Muon Lifetime and Determination of the Fermi Constant, Phys. Rev. D87, 052003 (2013), arXiv:1211.0960

  12. [12]

    Adhikariet al.(CREX), Precision Determination of the Neutral Weak Form Factor of 48Ca, Phys

    D. Adhikariet al.(CREX), Precision Determination of the Neutral Weak Form Factor of 48Ca, Phys. Rev. Lett. 129, 042501 (2022), arXiv:2205.11593

  13. [13]

    Abrahamyanet al.(PREX), Measurement of the Neutron Radius of 208Pb Through Parity-Violation in Electron Scattering, Phys

    S. Abrahamyanet al.(PREX), Measurement of the Neutron Radius of 208Pb Through Parity-Violation in Electron Scattering, Phys. Rev. Lett.108, 112502 (2012), arXiv:1201.2568

  14. [14]

    Adhikariet al.(PREX), Accurate Determination of the Neutron Skin Thickness of 208Pb through Parity- Violation in Electron Scattering, Phys

    D. Adhikariet al.(PREX), Accurate Determination of the Neutron Skin Thickness of 208Pb through Parity- Violation in Electron Scattering, Phys. Rev. Lett.126, 172502 (2021), arXiv:2102.10767

  15. [15]

    Androi´ cet al.( Qweak), Determination of the 27Al Neutron Distribution Radius from a Parity-Violating Electron Scattering Measurement, Phys

    D. Androi´ cet al.( Qweak), Determination of the 27Al Neutron Distribution Radius from a Parity-Violating Electron Scattering Measurement, Phys. Rev. Lett.128, 132501 (2022), arXiv:2112.15412

  16. [16]

    de Vries, C

    H. de Vries, C. W. de Jager, and C. de Vries, Nuclear charge and magnetization density distribution parame- ters from elastic electron scattering, Atom. Data Nucl. Data Tabl.36, 495 (1987)

  17. [17]

    C. J. Horowitz, Parity violating elastic electron scattering and Coulomb distortions, Phys. Rev. C57, 3430 (1998), arXiv:nucl-th/9801011

  18. [18]

    C. J. Horowitz, S. J. Pollock, P. A. Souder, and R. Michaels, Parity violating measurements of neutron densities, Phys. Rev. C63, 025501 (2001), arXiv:nucl- th/9912038

  19. [19]

    C. J. Horowitzet al., Weak charge form factor and radius of 208Pb through parity violation in electron scattering, Phys. Rev. C85, 032501 (2012), arXiv:1202.1468

  20. [20]

    C. J. Horowitz, Parity violating elastic electron scattering from 27Al and the Qweak measurement, Phys. Rev. C 89, 045503 (2014), arXiv:1401.6898

  21. [21]

    Reinhard, X

    P.-G. Reinhard, X. Roca-Maza, and W. Nazarewicz, Combined Theoretical Analysis of the Parity-Violating Asymmetry for 48Ca and 208Pb, Phys. Rev. Lett.129, 232501 (2022), arXiv:2206.03134

  22. [22]

    Y¨ uksel and N

    E. Y¨ uksel and N. Paar, Implications of parity-violating electron scattering experiments on 48Ca (CREX) and 208Pb (PREX-II) for nuclear energy density functionals, Phys. Lett. B836, 137622 (2023), arXiv:2206.06527

  23. [23]

    Zhang and L.-W

    Z. Zhang and L.-W. Chen, Bayesian inference of the symmetry energy and the neutron skin in 48Ca and 208Pb from CREX and PREX-2, Phys. Rev. C108, 024317 (2023), arXiv:2207.03328

  24. [24]

    Mondal and F

    C. Mondal and F. Gulminelli, Nucleonic metamodeling in light of multimessenger, PREX-II, and CREX data, Phys. Rev. C107, 015801 (2023), arXiv:2209.05177

  25. [25]

    Papakonstantinou, Nuclear Symmetry Energy and the PREX-CREX Neutron Skin Puzzle within the KIDS Framework, Nucl

    P. Papakonstantinou, Nuclear Symmetry Energy and the PREX-CREX Neutron Skin Puzzle within the KIDS Framework, Nucl. Theor.39, 36 (2022), 12 arXiv:2210.02696

  26. [26]

    Miyatsu, M.-K

    T. Miyatsu, M.-K. Cheoun, K. Kim, and K. Saito, Can the PREX-2 and CREX results be understood by relativistic mean-field models with the astrophys- ical constraints?, Phys. Lett. B843, 138013 (2023), arXiv:2303.14763

  27. [27]

    B. T. Reed, F. J. Fattoyev, C. J. Horowitz, and J. Piekarewicz, Density dependence of the symmetry energy in the post–PREX-CREX era, Phys. Rev. C109, 035803 (2024), arXiv:2305.19376

  28. [28]

    Sammarruca, The Neutron Skin of 48Ca and 208Pb: A Critical Analysis, Symmetry16, 34 (2024), arXiv:2311.02539

    F. Sammarruca, The Neutron Skin of 48Ca and 208Pb: A Critical Analysis, Symmetry16, 34 (2024), arXiv:2311.02539

  29. [29]

    T. Zhao, Z. Lin, B. Kumar, A. W. Steiner, and M. Prakash, Characterizing the nuclear models informed by PREX and CREX: A view from Bayesian inference, Phys. Rev. Res.7, 043335 (2025), arXiv:2406.05267

  30. [30]

    Roca-Maza and D

    X. Roca-Maza and D. H. Jakubassa-Amundsen, QED Corrections to the Parity-Violating Asymmetry in High- Energy Electron-Nucleus Collisions, Phys. Rev. Lett. 134, 192501 (2025), arXiv:2501.14375

  31. [31]

    Kunjipurayil, J

    A. Kunjipurayil, J. Piekarewicz, and M. Salinas, Role of the isovector spin-orbit potential in mitigating the CREX-PREX dilemma, Phys. Rev. C112, 014310 (2025), arXiv:2503.07405

  32. [32]

    B. T. Reed, M. Heinz, P. Arthuis, A. Schwenk, and I. Tews, Connecting relativistic density functional theory to microscopic calculations, Phys. Rev. C112, 034331 (2025), arXiv:2505.00828

  33. [33]

    B. T. Reed and C. J. Horowitz, Comment on QED Corrections to the Parity Violating Asymme- try in High-Energy Electron-Nucleus Scattering (2026), arXiv:2601.01615

  34. [34]

    Piekarewicz, The Matter Radius of 132Sn and the CREX-PREX Dilemma (2026), arXiv:2603.11983

    J. Piekarewicz, The Matter Radius of 132Sn and the CREX-PREX Dilemma (2026), arXiv:2603.11983

  35. [35]

    B. T. Reed and C. J. Horowitz, Electroweak Radiative Corrections to Parity-Violating Electron-Nucleus Scat- tering (2026), arXiv:2603.22581

  36. [36]

    Hagenet al., Neutron and weak-charge distribu- tions of the 48Ca nucleus, Nat

    G. Hagenet al., Neutron and weak-charge distribu- tions of the 48Ca nucleus, Nat. Phys.12, 186 (2015), arXiv:1509.07169

  37. [37]

    B. S. Huet al., Ab initio predictions link the neutron skin of 208Pb to nuclear forces, Nat. Phys.18, 1196 (2022), arXiv:2112.01125

  38. [38]

    Hebeler, V

    K. Hebeler, V. Durant, J. Hoppe, M. Heinz, A. Schwenk, J. Simonis, and A. Tichai, Normal ordering of three- nucleon interactions for ab initio calculations of heavy nu- clei, Phys. Rev. C107, 024310 (2023), arXiv:2211.16262

  39. [39]

    Arthuis, K

    P. Arthuis, K. Hebeler, and A. Schwenk, Neutron-rich nuclei and neutron skins from chiral low-resolution in- teractions (2024), arXiv:2401.06675

  40. [40]

    Bonaiti, G

    F. Bonaiti, G. Hagen, and T. Papenbrock, Structure of the doubly magic nuclei 208Pb and 266Pb from ab initio computations (2025), arXiv:2508.14217

  41. [41]

    Heinz, M

    M. Heinz, M. Hoferichter, T. Miyagi, F. No¨ el, and A. Schwenk, Ab initio calculations of overlap integrals for µ→e conversion in nuclei, Phys. Lett. B871, 139975 (2025), arXiv:2412.04545

  42. [42]

    Miyagi, M

    T. Miyagi, M. Heinz, and A. Schwenk, Ab initio com- putations of the fourth-order charge density moments of 48Ca and 208Pb, Phys. Lett. B872, 140032 (2026), arXiv:2508.10767

  43. [43]

    Hoferichter, P

    M. Hoferichter, P. Klos, J. Men´ endez, and A. Schwenk, Analysis strategies for general spin-independent WIMP- nucleus scattering, Phys. Rev. D94, 063505 (2016), arXiv:1605.08043

  44. [44]

    Hoferichter, P

    M. Hoferichter, P. Klos, J. Men´ endez, and A. Schwenk, Nuclear structure factors for general spin-independent WIMP-nucleus scattering, Phys. Rev. D99, 055031 (2019), arXiv:1812.05617

  45. [45]

    C. G. Payne, S. Bacca, G. Hagen, W. G. Jiang, and T. Papenbrock, Coherent elastic neutrino-nucleus scat- tering on 40Ar from first principles, Phys. Rev. C100, 061304 (2019), arXiv:1908.09739

  46. [46]

    Hoferichter, J

    M. Hoferichter, J. Men´ endez, and A. Schwenk, Coherent elastic neutrino-nucleus scattering: EFT analysis and nuclear responses, Phys. Rev. D102, 074018 (2020), arXiv:2007.08529

  47. [47]

    Hoferichter, J

    M. Hoferichter, J. Men´ endez, and F. No¨ el, Improved Limits on Lepton-Flavor-Violating Decays of Light Pseudoscalars via Spin-Dependent µ→e Conver- sion in Nuclei, Phys. Rev. Lett.130, 131902 (2023), arXiv:2204.06005

  48. [48]

    Hebeler, S

    K. Hebeler, S. K. Bogner, R. J. Furnstahl, A. Nogga, and A. Schwenk, Improved nuclear matter calculations from chiral low-momentum interactions, Phys. Rev. C 83, 031301 (2011), arXiv:1012.3381

  49. [49]

    W. G. Jiang, A. Ekstr¨ om, C. Forss´ en, G. Hagen, G. R. Jansen, and T. Papenbrock, Accurate bulk properties of nuclei from A = 2 to ∞ from potentials with ∆ isobars, Phys. Rev. C102, 054301 (2020), arXiv:2006.16774

  50. [50]

    Epelbaum, H.-W

    E. Epelbaum, H.-W. Hammer, and U.-G. Meißner, Mod- ern Theory of Nuclear Forces, Rev. Mod. Phys.81, 1773 (2009), arXiv:0811.1338

  51. [51]

    Machleidt and D

    R. Machleidt and D. R. Entem, Chiral effective field theory and nuclear forces, Phys. Rep.503, 1 (2011), arXiv:1105.2919

  52. [52]

    Hergert, S

    H. Hergert, S. K. Bogner, T. D. Morris, A. Schwenk, and K. Tsukiyama, The In-Medium Similarity Renor- malization Group: A Novel Ab Initio Method for Nuclei, Phys. Rep.621, 165 (2016), arXiv:1512.06956

  53. [53]

    Heinz, A

    M. Heinz, A. Tichai, J. Hoppe, K. Hebeler, and A. Schwenk, In-medium similarity renormalization group with three-body operators, Phys. Rev. C103, 044318 (2021), arXiv:2102.11172

  54. [54]

    No¨ el and M

    F. No¨ el and M. Hoferichter, Uncertainty quantification for µ →e conversion in nuclei: charge distributions, J. High Energy Phys.08(2024), 052, arXiv:2406.06677

  55. [55]

    No¨ el,µ →e conversion in nuclei: EFT description, charge densities, and pseudo-scalar decays, Ph.D

    F. No¨ el,µ →e conversion in nuclei: EFT description, charge densities, and pseudo-scalar decays, Ph.D. thesis, Bern U. (2024)

  56. [56]

    No¨ el,https://pypi.org/project/phasr/(2025)

    F. No¨ el,https://pypi.org/project/phasr/(2025)

  57. [57]

    Kl¨ upfel, P.-G

    P. Kl¨ upfel, P.-G. Reinhard, T. J. B¨ urvenich, and J. A. Maruhn, Variations on a theme by Skyrme: A systematic study of adjustments of model parameters, Phys. Rev. C79, 034310 (2009), arXiv:0804.3385

  58. [58]

    Erler, P

    J. Erler, P. Kl¨ upfel, and P.-G. Reinhard, Exploration of a modified density dependence in the Skyrme functional, Phys. Rev. C82, 044307 (2010), arXiv:1009.0624

  59. [59]

    Nazarewicz, P.-G

    W. Nazarewicz, P.-G. Reinhard, W. Satu la, and D. Vrete- nar, Symmetry energy in nuclear density functional the- ory, Eur. Phys. J. A50, 20 (2014), arXiv:1307.5782

  60. [60]

    Fricke, C

    G. Fricke, C. Bernhardt, K. Heilig, L. A. Schaller, L. Schellenberg, E. B. Shera, and C. W. de Jager, Nuclear Ground State Charge Radii from Electromagnetic Inter- actions, Atom. Data Nucl. Data Tabl.60, 177 (1995)

  61. [61]

    Z. Sun, K. A. Beyer, Z. A. Mandrykina, I. A. Val- uev, C. H. Keitel, and N. S. Oreshkina, 208Pb Nuclear 13 Charge Radius Revisited: Closing the Fine-Structure- Anomaly Gap, Phys. Rev. Lett.135, 163002 (2025), arXiv:2504.19977

  62. [62]

    Beckeret al., The P2 experiment, Eur

    D. Beckeret al., The P2 experiment, Eur. Phys. J. A 54, 208 (2018), arXiv:1802.04759

  63. [63]

    Heinz, T

    M. Heinz, T. Miyagi, S. R. Stroberg, A. Tichai, K. Hebeler, and A. Schwenk, Improved structure of cal- cium isotopes from ab initio calculations, Phys. Rev. C 111, 034311 (2025), arXiv:2411.16014

  64. [64]

    J. B. Bellicard and K. J. van Oostrum, Elastic Electron Scattering from Lead-208 at 175 and 250 MeV, Phys. Rev. Lett.19, 242 (1967)

  65. [65]

    G. J. C. Van Niftrik, Elastic scattering of electrons from lead and bismuth at 40 to 60 MeV, Nucl. Phys. A131, 574 (1969)

  66. [66]

    Heisenberg, R

    J. Heisenberg, R. Hofstadter, J. S. McCarthy, I. Sick, B. C. Clark, R. Herman, and D. G. Ravenhall, Elas- tic Electron Scattering by 208Pb And New Information About the Nuclear Charge Distribution, Phys. Rev. Lett. 23, 1402 (1969)

  67. [67]

    Nagao and Y

    M. Nagao and Y. Torizuka, Electron excitation of low- lying states in 208Pb, Phys. Lett. B37, 383 (1971)

  68. [68]

    Friedrich and F

    J. Friedrich and F. Lenz, Elastic electron scattering from 208Pb at moderate momentum transfers and model- independent description of the nuclear charge distribu- tion, Nucl. Phys. A183, 523 (1972)

  69. [69]

    J. L. Friar and J. W. Negele, The determination of the nuclear charge distribution of 208Pb from elastic electron scattering and muonic X-rays, Nucl. Phys. A212, 93 (1973)

  70. [70]

    Dreher, J

    B. Dreher, J. Friedrich, K. Merle, H. Rothhaas, and G. L¨ uhrs, The determination of the nuclear ground state and transition charge density from measured electron scattering data, Nucl. Phys. A235, 219 (1974)

  71. [71]

    C. W. de Jager, H. de Vries, and C. de Vries, Nuclear charge and magnetization density distribution parame- ters from elastic electron scattering, Atom. Data Nucl. Data Tabl.14, 479 (1974), [Erratum: Atom. Data Nucl. Data Tabl.16, 580 (1975)]

  72. [72]

    Euteneuer, J

    H. Euteneuer, J. Friedrich, and N. Voegler, Charge Dis- tribution of 208Pb and the Difference in ρ(r) for Pb and Tl Investigated by by Elastic Electron Scattering, Phys. Rev. Lett.36, 129 (1976)

  73. [73]

    H. Euteneuer,Elastische Elektronenstreuung an 208Pb und seinen Nachbarkernen 209Bi, 207,206,204Pb sowie 205,203Tl zur Bestimmung der Grundzustand- sladungsverteilung dieser Nuklide, Ph.D. thesis, Johannes-Gutenberg-Universit¨ at Mainz (1976)

  74. [74]

    Frois, J

    B. Frois, J. B. Bellicard, J. M. Cavedon, M. Huet, P. Leconte, P. Ludeau, A. Nakada, X. H. Phan, and I. Sick, High Momentum Transfer electron Scattering from 208Pb, Phys. Rev. Lett.38, 152 (1977)

  75. [75]

    Euteneuer, J

    H. Euteneuer, J. Friedrich, and N. Voegler, What can be learnt about nuclear polarization from a consistency analysis of e−cross sections and muonic X-rays for 208Pb and the isotone pair 209Bi/208Pb?, Z. Physik A280, 165 (1977)

  76. [76]

    Euteneuer, J

    H. Euteneuer, J. Friedrich, and N. Vogler, The Charge Distribution Differences of 209Bi, 208,207,206,204Pb and 205,203Tl Investigated by Elastic electron Scattering and Muonic X-Ray Data, Nucl. Phys. A298, 452 (1978)

  77. [77]

    P. Mazanek,Gemeinsame Auswertung von Messun- gen myonischer Atome, optischer Isotopieverschiebun- gen und elastischer Elektronenstreuung zur Festlegung von Radien stabiler und instabiler Kerne unterhalb von N = 126sowie Bestimmung von Kernradien aus µ- Atom-Messungen f¨ ur Erbium- und Wolframisotope, Ph.D. thesis, Johannes-Gutenberg-Universit¨ at Mainz (1992)

  78. [78]

    Gorchtein and C

    M. Gorchtein and C. J. Horowitz, Dispersion γZ-box correction to the weak charge of the proton, Phys. Rev. Lett.102, 091806 (2009), arXiv:0811.0614

  79. [79]

    Gorchtein, C

    M. Gorchtein, C. J. Horowitz, and M. J. Ramsey-Musolf, Model-dependence of the γZ dispersion correction to the parity-violating asymmetry in elastic ep scattering, Phys. Rev. C84, 015502 (2011), arXiv:1102.3910

  80. [80]

    Androi´ cet al.( Qweak), Precision measurement of the weak charge of the proton, Nature557, 207 (2018), arXiv:1905.08283

    D. Androi´ cet al.( Qweak), Precision measurement of the weak charge of the proton, Nature557, 207 (2018), arXiv:1905.08283

Showing first 80 references.