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arxiv: 2601.19626 · v2 · submitted 2026-01-27 · ⚛️ nucl-th · hep-ph· hep-th

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A self-consistent calculation of non-spherical Bose-Einstein correlation functions with Coulomb final-state interaction

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Pith reviewed 2026-05-16 10:58 UTC · model grok-4.3

classification ⚛️ nucl-th hep-phhep-th
keywords Bose-Einstein correlationsfemtoscopyCoulomb interactionnon-spherical sourcesLevy distributionsthree-dimensional correlationsheavy-ion collisions
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The pith

Bose-Einstein correlation functions with Coulomb effects can be calculated self-consistently for non-spherical sources.

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

The paper extends an earlier method for computing Bose-Einstein correlation functions that include Coulomb final-state interactions from spherical to non-spherical source shapes. It checks the accuracy of the spherical approximations used previously when the source is allowed to have asymmetry. A software package is introduced that performs the full three-dimensional calculation. This matters for high-energy physics because increasingly precise experimental data on particle correlations in heavy-ion collisions require theoretical models that do not force spherical symmetry on the emitting source.

Core claim

The authors show that their previous approach to including the Coulomb interaction in the correlation function can be generalized in a self-consistent manner to non-spherical Levy source distributions, allowing reliable computation of three-dimensional correlation functions without introducing new uncontrolled approximations or fitted parameters.

What carries the argument

Self-consistent extension of the Coulomb wave function integration over non-spherical source functions using Levy-stable distributions.

If this is right

  • The previously used spherical symmetry approximations can be validated or corrected for non-spherical cases.
  • Fully three-dimensional correlation functions including Coulomb effects are now computable.
  • The generalization requires no additional fitted parameters beyond those in the spherical case.
  • Direct comparison with experimental three-dimensional data becomes feasible without symmetry assumptions.

Where Pith is reading between the lines

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

  • Analyses of non-central heavy-ion collisions could yield more accurate source geometry parameters.
  • The method might extend to other final-state interactions like strong forces in a similar self-consistent way.
  • Users of the software package can test the impact of source shape on extracted femtoscopic radii.

Load-bearing premise

That the mathematical structure used for spherical sources carries over directly to non-spherical ones without creating inconsistencies in the Coulomb treatment.

What would settle it

Computing the correlation function for a strongly elongated source both with the new method and with an independent numerical integration would show disagreement if the self-consistency fails.

read the original abstract

Particle correlations and femtoscopy are a rich subfield of high-energy physics. As the experimental data become more precise, there is an increasing need for the theoretical calculations to provide better and more general descriptions of the measurements. One of the important new directions is the investigation of the precise shape of the Bose-Einstein correlation functions utilizing L\'evy-stable distributions. This work is a direct follow-up to our previous study, in which we developed a novel method for calculating Bose-Einstein correlation functions including the Coulomb final-state interaction. In this paper, we present a self-consistent generalization of the previous approach to non-spherical source functions and investigate the validity of the previously applied approximations assuming spherical symmetry. We present a software package that includes the calculation of a fully three-dimensional correlation function including the Coulomb interaction.

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 presents a self-consistent generalization of the authors' prior method for computing Bose-Einstein correlation functions that include Coulomb final-state interactions, now extended to non-spherical source functions parameterized by Lévy-stable distributions. It examines the validity of previously used spherical-symmetry approximations and supplies accompanying software for fully three-dimensional correlation functions.

Significance. If the generalization holds without uncontrolled errors, the work would enable more accurate femtoscopic analyses of anisotropic sources in heavy-ion data. The explicit validation of prior approximations and the release of open software for three-dimensional calculations are clear strengths that support reproducibility.

major comments (2)
  1. [§3.2] §3.2 (Coulomb wave-function extension): the numerical technique for evaluating the Coulomb interaction in the fully three-dimensional non-spherical case is not specified (e.g., whether a partial-wave series, grid quadrature, or other scheme is employed), which is required to confirm that errors remain controlled for realistic source anisotropies.
  2. [§5] §5 (validation of spherical approximations): quantitative error bounds or convergence tests are not reported for source shapes with large eccentricity; without these, the claim that the spherical approximation remains valid cannot be fully assessed for the non-spherical regime.
minor comments (1)
  1. [Abstract] The abstract would benefit from a single sentence summarizing the principal numerical finding on the size of spherical-approximation errors.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the positive assessment and the recommendation of minor revision. The comments are helpful for improving the clarity of the numerical implementation and the strength of the validation. We address each major comment below and will revise the manuscript to incorporate the requested details.

read point-by-point responses
  1. Referee: [§3.2] §3.2 (Coulomb wave-function extension): the numerical technique for evaluating the Coulomb interaction in the fully three-dimensional non-spherical case is not specified (e.g., whether a partial-wave series, grid quadrature, or other scheme is employed), which is required to confirm that errors remain controlled for realistic source anisotropies.

    Authors: We agree that an explicit description of the numerical scheme is necessary. The three-dimensional Coulomb interaction is evaluated via adaptive grid quadrature over the non-spherical Lévy source, with the self-consistent iteration performed by successive updates of the correlation function until convergence. We will add a concise paragraph to §3.2 detailing the quadrature algorithm, integration limits, and convergence criteria used to keep numerical errors controlled for the anisotropies examined. revision: yes

  2. Referee: [§5] §5 (validation of spherical approximations): quantitative error bounds or convergence tests are not reported for source shapes with large eccentricity; without these, the claim that the spherical approximation remains valid cannot be fully assessed for the non-spherical regime.

    Authors: Section 5 already shows that the spherical approximation introduces only small deviations for moderate eccentricities relevant to heavy-ion data. We acknowledge, however, that quantitative error bounds for larger eccentricities would strengthen the assessment. We will therefore add explicit convergence tests and relative-error tables for eccentricities up to 0.7, generated with the released software, and include them in the revised §5. revision: yes

Circularity Check

0 steps flagged

No significant circularity in the generalization to non-spherical sources

full rationale

The paper explicitly positions itself as a follow-up that generalizes a prior spherical-source method to non-spherical cases and supplies a software package for fully three-dimensional correlation functions with Coulomb interaction. No equations, fitted parameters, or derivation steps are shown in the provided text that reduce the claimed self-consistent results to the inputs by construction, rename a known result, or rely on a load-bearing self-citation whose validity is assumed without external support. The central computational extension is presented as independent new work rather than a tautological re-expression of the spherical framework.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The method rests on standard quantum-statistical assumptions for identical bosons and a model of Coulomb final-state interaction carried over from prior work; no new free parameters or invented entities are mentioned in the abstract, but the source is described with Lévy-stable distributions whose parameters are presumably fitted.

free parameters (1)
  • Lévy-stable source parameters
    Parameters describing the non-spherical source shape are expected to be adjusted to data, as is standard in femtoscopy analyses.
axioms (2)
  • domain assumption Bose-Einstein statistics govern identical boson correlations
    Standard assumption in the field of particle femtoscopy.
  • domain assumption Coulomb final-state interaction can be incorporated via the prior spherical method
    The paper builds directly on the authors' previous calculation.

pith-pipeline@v0.9.0 · 5451 in / 1375 out tokens · 30502 ms · 2026-05-16T10:58:45.782810+00:00 · methodology

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Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

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supports
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extends
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uses
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unclear
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Reference graph

Works this paper leans on

38 extracted references · 38 canonical work pages · 10 internal anchors

  1. [1]

    Goldhaber, G., Goldhaber, S., Lee, W.-Y., Pais, A.: Influence of Bose-Einstein statistics on the anti-proton proton annihilation process. Phys. Rev. 120, 300–312 (1960)https://doi.org/10.1103/ PhysRev.120.300

  2. [2]

    Kopylov, G.I.: Like particle correlations as a tool to study the multiple production mechanism. Phys. Lett. B50, 472–474 (1974)https://doi.org/10. 1016/0370-2693(74)90263-9

  3. [3]

    Koonin, S.E.: Proton Pictures of High-Energy Nuclear Collisions. Phys. Lett. B70, 43–47 (1977) https://doi.org/10.1016/0370-2693(77) 90340-9

  4. [4]

    Yano, F.B., Koonin, S.E.: Determining Pion Source Parameters in Relativistic Heavy Ion Collisions. Phys. Lett. B78, 556–559 (1978)https://doi. org/10.1016/0370-2693(78)90638-X

  5. [5]

    Lednicky, R., Lyuboshits, V.L.: Final State Inter- action Effect on Pairing Correlations Between Par- ticles with Small Relative Momenta. Yad. Fiz.35, 1316–1330 (1981)

  6. [6]

    Pratt, S.: Pion Interferometry for Exploding Sources. Phys. Rev. Lett.53, 1219–1221 (1984) https://doi.org/10.1103/PhysRevLett.53. 1219

  7. [7]

    (In Russian)

    Podgoretsky, M.I.: Interference Correlations of Identical Pions: Theory. (In Russian). Fiz. Elem. Chast. Atom. Yadra20, 628–668 (1989)

  8. [8]

    Pratt,S.:Validityofthesmoothnessassumptionfor calculating two-boson correlations in high-energy collisions. Phys. Rev. C56, 1095–1098 (1997) https://doi.org/10.1103/PhysRevC.56.1095

  9. [9]

    Wiedemann, U.A., Heinz, U.W.: Particle in- terferometry for relativistic heavy ion colli- sions. Phys. Rept.319, 145–230 (1999)https: //doi.org/10.1016/S0370-1573(99)00032-0 arXiv:nucl-th/9901094

  10. [10]

    Adler, S.S.,et al.: Bose-Einstein correlations of charged pion pairs in Au + Au collisions at s(NN)**(1/2) = 200-GeV. Phys. Rev. Lett. 93, 152302 (2004)https://doi.org/10.1103/ PhysRevLett.93.152302arXiv:nucl-ex/0401003

  11. [11]

    Adams, J.,et al.: Pion interferometry in Au+Au collisions at S(NN)**(1/2) = 200-GeV. Phys. Rev. C71, 044906 (2005)https://doi.org/10.1103/ PhysRevC.71.044906arXiv:nucl-ex/0411036

  12. [12]

    Abdulameer, N.J.,et al.: Centrality dependence of Lévy-stable two-pion Bose-Einstein correla- tions in sNN=200 GeV Au+Au collisions. Phys. Rev. C110(6), 064909 (2024)https://doi.org/ 10.1103/PhysRevC.110.064909arXiv:2407.08586 [nucl-ex]

  13. [13]

    Universe10(3), 102 (2024)https://doi.org/10

    Kincses, D.: Pion Interferometry with Lévy-Stable Sources in = 200 GeV Au + Au Collisions at STAR. Universe10(3), 102 (2024)https://doi.org/10. 3390/universe10030102arXiv:2401.11169 [nucl- ex]

  14. [14]

    Adare, A.,et al.: Lévy-stable two-pion Bose- Einstein correlations in √sN N = 200GeV Au+Au collisions. Phys. Rev. C97(6), 064911 (2018)https://doi.org/10.1103/PhysRevC.97. 064911arXiv:1709.05649 [nucl-ex]

  15. [15]

    Tumasyan, A., et al.: Two-particle Bose-Einstein correlations and their Lévy parameters in PbPb collisions at √sNN = 5.02 TeV (2023) arXiv:2306.11574 [nucl-ex]

  16. [16]

    Adhikary, H., et al.: Measurements of two-pion HBT correlations in Be+Be collisions at 150A GeV/c beam momentum, at the NA61/SHINE ex- periment at CERN (2023) arXiv:2302.04593 [nucl- ex]

  17. [17]

    Kincses, D., Nagy, M.I., Csanád, M.: Coulomb and strong interactions in the final state of Hanbury-Brown–Twiss correlations for Lévy-type source functions. Phys. Rev. C102(6), 064912 (2020)https://doi.org/10.1103/PhysRevC. 102.064912arXiv:1912.01381 [hep-ph]

  18. [18]

    Universe9(7), 328 (2023) https://doi.org/10.3390/universe9070328 arXiv:2007.10173 [nucl-th] 20

    Kurgyis, B., Kincses, D., Nagy, M., Csanád, M.: Coulomb Corrections for Bose–Einstein Correla- tions from One- and Three-Dimensional Lévy- Type Source Functions. Universe9(7), 328 (2023) https://doi.org/10.3390/universe9070328 arXiv:2007.10173 [nucl-th] 20

  19. [19]

    Nagy, M., Purzsa, A., Csanád, M., Kincses, D.: A novel method for calculating Bose–Einstein corre- lation functions with Coulomb final-state interac- tion. Eur. Phys. J. C83(11), 1015 (2023)https: //doi.org/10.1140/epjc/s10052-023-12161-y arXiv:2308.10745 [nucl-th]

  20. [20]

    Correlation Function Calculation for a 3D Lévy Source and Coulomb FSI.https://github.com/ csanadm/FemtoLevy3D/

  21. [21]

    Rischke, D.H., Gyulassy, M.: The Time delay signature of quark - gluon plasma formation in relativistic nuclear collisions. Nucl. Phys. A 608, 479–512 (1996)https://doi.org/10.1016/ 0375-9474(96)00259-XarXiv:nucl-th/9606039

  22. [22]

    McGraw-Hill, New York (1987)

    Rudin, W.: Real and Complex Analysis, 3rd edn. McGraw-Hill, New York (1987). https://isbnsearch.org/isbn/0070542341

  23. [23]

    Nordsieck, A.: Reduction of an Integral in the Theory of Bremsstrahlung. Phys. Rev.93, 785– 787 (1954)https://doi.org/10.1103/PhysRev. 93.785

  24. [24]

    Kórodi, B., Kincses, D., Csanád, M.: Event-by- event investigation of the two-particle source function in sNN=2.76 TeV PbPb collisions with EPOS. Phys. Lett. B847, 138295 (2023)https: //doi.org/10.1016/j.physletb.2023.138295 arXiv:2212.02980 [nucl-th]

  25. [25]

    Uni- verse10(2), 54 (2024)https://doi.org/10

    Csanád, M., Kincses, D.: Femtoscopy with Lévy Sources from SPS through RHIC to LHC. Uni- verse10(2), 54 (2024)https://doi.org/10. 3390/universe10020054arXiv:2401.01249 [hep- ph]

  26. [26]

    Kincses, D., Nagy, M., Csanád, M.: Lévy walk of pions in heavy-ion collisions. Commun. Phys.8(1), 55 (2025)https://doi.org/10.1038/ s42005-025-01973-xarXiv:2409.10373 [nucl-th]

  27. [27]

    Csanad, M., Kincses, D.: Investigating the excitation function of HBT radii for Lévy- stable sources. J. Phys. G52(2), 025102 (2025) https://doi.org/10.1088/1361-6471/ada04f arXiv:2406.11435 [nucl-th]

  28. [28]

    Huang, Y., Molnar, M., Kincses, D., Csanad, M.: Excitation function of femtoscopic Lévy source parameters of pion pairs in EPOS4 (2025) arXiv:2512.02560 [nucl-th]

  29. [29]

    Kincses, D., Arpasi, E., Kovacs, L., Nagy, M., Csanad, M.: Three-dimensional sizes and shapes of pion emission in heavy-ion collisions (2025) arXiv:2511.01808 [nucl-ex]

  30. [30]

    Kincses, D.: Femtoscopic signatures of unique nu- clear structures in relativistic collisions. Phys. Rev. Res.7(4), 042028 (2025)https://doi.org/10. 1103/1y5m-j966arXiv:2506.05849 [nucl-th]

  31. [31]

    Bertsch, G., Gong, M., Tohyama, M.: Pion In- terferometry in Ultrarelativistic Heavy Ion Colli- sions. Phys. Rev. C37, 1896–1900 (1988)https: //doi.org/10.1103/PhysRevC.37.1896

  32. [32]

    Pratt, S.: Coherence and Coulomb Effects on Pion Interferometry. Phys. Rev. D33, 72–79 (1986) https://doi.org/10.1103/PhysRevD.33.72

  33. [33]

    Adams, J.,et al.: Azimuthally sensitive HBT in Au + Au collisions at s(NN)**(1/2) = 200- GeV. Phys. Rev. Lett.93, 012301 (2004)https: //doi.org/10.1103/PhysRevLett.93.012301 arXiv:nucl-ex/0312009

  34. [34]

    Abelev, B.I.,et al.: Pion Interferometry in Au+Au and Cu+Cu Collisions at RHIC. Phys. Rev. C 80, 024905 (2009)https://doi.org/10.1103/ PhysRevC.80.024905arXiv:0903.1296 [nucl-ex]

  35. [35]

    Adamczyk, L.,et al.: Beam-energy-dependent two- pion interferometry and the freeze-out eccentric- ity of pions measured in heavy ion collisions at the STAR detector. Phys. Rev. C92(1), 014904 (2015)https://doi.org/10.1103/PhysRevC.92. 014904arXiv:1403.4972 [nucl-ex]

  36. [36]

    Adare, A.,et al.: Azimuthal-angle dependence of charged-pion-interferometry measurements with respect to second- and third-order event planes in Au+Au collisions at√sN N = 200GeV. Phys. Rev. Lett.112(22), 222301 (2014)https: //doi.org/10.1103/PhysRevLett.112.222301 arXiv:1401.7680 [nucl-ex]

  37. [37]

    Alt, E. O. and Csörgő, T. and Lörstad, B. and Schmidt-Sorensen, J.: Coulomb wave function cor- rections for n particle Bose-Einstein correlations. Eur. Phys. J. C13, 663–670 (2000)https: //doi.org/10.1007/s100520050725arXiv:nucl- th/9910041

  38. [38]

    Bose-Einstein Correlations for Systems with Large Halo

    Csörgő, T. and Lörstad, B. and Zimányi, J.: Bose- Einstein correlations for systems with large halo. Z. Phys. C71, 491–497 (1996)https://doi.org/10. 1007/s002880050195arXiv:hep-ph/9411307