pith. machine review for the scientific record. sign in

arxiv: 2604.08667 · v1 · submitted 2026-04-09 · ✦ hep-ph

Recognition: unknown

On Exclusive Coherent Production of Bosons in Electron-Proton Collisions

Authors on Pith no claims yet

Pith reviewed 2026-05-10 16:51 UTC · model grok-4.3

classification ✦ hep-ph
keywords exclusive electroproductionforward proton kinematicsElectron-Ion Collideraxion-like particlesdark photonsmeson productionphenomenological amplitudesequivalent photon approximation
0
0 comments X

The pith

A unified 2-to-3 framework supplies full kinematics for exclusive production of mesons, axion-like particles and dark photons in electron-proton collisions at the EIC.

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

The paper develops a single framework for the exclusive electroproduction process e + p to e' + p' + X in the forward-proton kinematics planned for the Electron-Ion Collider. The framework uses phenomenological amplitudes fitted to existing photo- and electroproduction data and treats pseudoscalar and vector mesons together with axion-like particles and vector mediators such as dark photons. It supplies the complete three-body kinematics rather than relying on flux-factorized approximations. A sympathetic reader would care because the approach makes concrete predictions for total rates, differential distributions and missing-proton-energy signatures that can guide detector acceptance and signal selection at the EIC.

Core claim

The authors establish that a unified 2 to 3 kinematic framework, constructed from phenomenological amplitudes constrained by existing data, provides the full event kinematics for exclusive coherent production of bosons in electron-proton collisions. Benchmark comparisons show close agreement with equivalent-photon-approximation descriptions for total rates and single-differential distributions in the near-real-photon regime, while finite photon virtuality introduces important correlations in multi-differential observables at larger Q squared. A detailed study of the missing-proton-energy signature demonstrates how the full treatment informs forward-proton acceptance and signal selection in E

What carries the argument

The unified 2-to-3 framework that supplies complete event kinematics from phenomenological amplitudes constrained by photo- and electroproduction data.

If this is right

  • Total rates and single-differential distributions agree closely with equivalent-photon-approximation results in the near-real-photon regime.
  • Finite-Q squared correlations become essential for accurate multi-differential observables once photon virtuality increases.
  • The missing-proton-energy signature directly informs forward-proton acceptance cuts and background rejection in realistic EIC detector geometries.
  • The framework is constructed to admit systematic refinement when new photo- or electroproduction data appear.

Where Pith is reading between the lines

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

  • The same amplitude-based structure could be applied to exclusive processes at other lepton-hadron facilities to test consistency across energy ranges.
  • It supplies a concrete starting point for estimating signal-to-background ratios in light new-physics searches that rely on missing-mass or missing-energy signatures.
  • Polarization observables or higher-order virtuality corrections could be added later without changing the overall 2-to-3 structure.

Load-bearing premise

The phenomenological amplitudes constrained by existing photo- and electroproduction data accurately describe the processes in the forward-proton kinematics and at the photon virtualities relevant for the EIC.

What would settle it

A precision measurement of multi-differential cross sections or missing-proton-energy distributions in exclusive production at the EIC that deviates from the framework predictions after detector simulation would show that the amplitudes do not extrapolate correctly to the relevant kinematics.

Figures

Figures reproduced from arXiv: 2604.08667 by Alexander Jentsch, Hongkai Liu, Maksym Ovchynnikov, Reuven Balkin, Sokratis Trifinopoulos, Ta'el Coren, Yotam Soreq.

Figure 1
Figure 1. Figure 1: FIG. 1. Feynman diagrams for the electroproduction process [PITH_FULL_IMAGE:figures/full_fig_p012_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Feynman diagrams for exclusive electroproduction of vector mesons [PITH_FULL_IMAGE:figures/full_fig_p014_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. The differential cross-section [PITH_FULL_IMAGE:figures/full_fig_p017_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Comparison between the analytic (red) and Monte-Carlo sampler (blue) implementations of the full 2 [PITH_FULL_IMAGE:figures/full_fig_p019_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. The differential distributions of the [PITH_FULL_IMAGE:figures/full_fig_p021_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. The distribution [PITH_FULL_IMAGE:figures/full_fig_p022_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. The electroproduction cross-sections after the selection in Eqs. (76)-(78), for the energy beam configurations [PITH_FULL_IMAGE:figures/full_fig_p023_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. The production cross-section of ALPs, [PITH_FULL_IMAGE:figures/full_fig_p023_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: FIG. 9. The differential cross-sections for the coherent production process (1), as obtained by the 2 [PITH_FULL_IMAGE:figures/full_fig_p025_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: FIG. 10. Comparison of the differential cross-sections of the pion photoproduction, as obtained following the [PITH_FULL_IMAGE:figures/full_fig_p033_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: FIG. 11. The differential cross-section [PITH_FULL_IMAGE:figures/full_fig_p034_11.png] view at source ↗
read the original abstract

We study the exclusive electroproduction process $e+p\to e'+p'+X$, with $X$ a single-particle final state, in the forward-proton kinematics relevant for the future Electron-Ion Collider (EIC). We develop a unified $2\to 3$ framework that provides the full event kinematics and incorporates pseudoscalar and vector mesons, as well as axion-like particles and vector mediators such as dark photons. It is based on phenomenological amplitudes constrained by existing photo- and electroproduction data and constructed to admit systematic refinement as new measurements become available. To benchmark the framework, we compare its predictions to flux-factorized descriptions based on the equivalent-photon approximation, demonstrating close agreement for total rates and selected single-differential distributions in the near-real regime, while highlighting the role of finite-$Q^{2}$ correlations for multi-differential observables at larger photon virtualities. As a case study, we perform a detailed kinematic analysis of the missing-proton-energy signature, illustrating how the full $2\to 3$ treatment informs forward-proton acceptance and signal selection in realistic EIC configurations.

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 paper develops a unified 2→3 framework for exclusive coherent electroproduction e+p→e'+p'+X (X = pseudoscalar/vector mesons, ALPs, dark photons) in forward-proton kinematics at EIC energies. The framework employs phenomenological amplitudes constrained by existing photo- and electroproduction data, supplies full event kinematics, and is benchmarked against flux-factorized equivalent-photon-approximation predictions, showing close agreement for total rates and single-differential distributions near the real-photon limit while noting finite-Q² correlations at larger virtualities. A case study on missing-proton-energy signatures for signal selection is included.

Significance. If the amplitudes remain accurate under extrapolation to low |t| and moderate-to-high Q² with the virtual-photon polarization structure of the 2→3 process, the work supplies a practical tool for EIC acceptance studies and background estimation that includes both SM mesons and BSM mediators. The explicit provision of full kinematics, the design for systematic refinement, and the direct comparison to EPA (rather than purely theoretical amplitudes) are concrete strengths that would aid experimental planning.

major comments (2)
  1. [§3] §3 (phenomenological amplitudes): The explicit functional forms of the amplitudes and the precise datasets used to constrain their parameters are not reported. Because the central claim of reliable predictions rests on the accuracy of these amplitudes when extrapolated to the forward-proton, finite-Q² EIC regime, the absence of these details prevents independent reproduction or quantitative assessment of extrapolation uncertainty.
  2. [§4] §4 (benchmarking): Agreement with the equivalent-photon approximation is stated for total rates and selected single-differential distributions in the near-real-photon limit, but no χ² values, error bands, or quantitative measures of discrepancy are given for the multi-differential observables at larger Q² where finite-Q² correlations are emphasized. This weakens the ability to judge the practical size of the reported differences.
minor comments (1)
  1. [Abstract] The abstract and introduction would benefit from a concise statement of the Q² range (e.g., 0.1–10 GeV²) over which the framework is claimed to be applicable and benchmarked.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the thorough review and the recommendation for minor revision. The comments have been helpful in identifying areas where the manuscript can be improved for clarity and reproducibility. We address each major comment below.

read point-by-point responses
  1. Referee: [§3] §3 (phenomenological amplitudes): The explicit functional forms of the amplitudes and the precise datasets used to constrain their parameters are not reported. Because the central claim of reliable predictions rests on the accuracy of these amplitudes when extrapolated to the forward-proton, finite-Q² EIC regime, the absence of these details prevents independent reproduction or quantitative assessment of extrapolation uncertainty.

    Authors: We appreciate the referee highlighting this issue. While §3 of the manuscript describes the structure of the phenomenological amplitudes and references the relevant photo- and electroproduction data used for constraints, the explicit functional forms (such as the specific parametrizations for the t-dependence and Q² evolution) and the precise list of datasets were not provided in full detail. In the revised manuscript, we will include these explicit forms in a new appendix and enumerate the datasets (e.g., specific HERA measurements for ρ and φ production, and JLab data for π⁰ and η). This will enable independent reproduction and better evaluation of extrapolation uncertainties to the EIC kinematics. We have also expanded the discussion in §3 to address potential uncertainties in the forward limit. revision: yes

  2. Referee: [§4] §4 (benchmarking): Agreement with the equivalent-photon approximation is stated for total rates and selected single-differential distributions in the near-real-photon limit, but no χ² values, error bands, or quantitative measures of discrepancy are given for the multi-differential observables at larger Q² where finite-Q² correlations are emphasized. This weakens the ability to judge the practical size of the reported differences.

    Authors: We agree that additional quantitative information would aid in assessing the differences. The manuscript presents the comparisons primarily through figures showing overlaid distributions to demonstrate the close agreement near Q²=0 and the emergence of finite-Q² effects. To address this, in the revision we will add error bands to the plots based on the uncertainties in the amplitude parameters and include a supplementary table providing quantitative measures, such as the percentage differences for integrated rates and key differential bins at various Q² values. While computing full χ² values for all multi-differential observables is beyond the scope of this phenomenological study (as it would require a global fit to all data), we believe the added metrics will allow readers to judge the practical size of the reported differences more effectively. revision: partial

Circularity Check

0 steps flagged

No circularity; phenomenological amplitudes are inputs, not outputs of the derivation

full rationale

The manuscript states that its unified 2→3 framework 'is based on phenomenological amplitudes constrained by existing photo- and electroproduction data' and is 'constructed to admit systematic refinement'. It then benchmarks total rates and single-differential distributions against the equivalent-photon approximation in the near-real-photon limit, noting differences at finite Q². No equation or step is shown that reduces the reported EIC kinematics, missing-energy distributions, or multi-differential predictions to the input fits by algebraic identity or by re-labeling a fitted parameter as a 'prediction'. The comparison to the EPA is an external cross-check rather than an internal tautology. Self-citations, if present for the amplitude parametrizations, are not load-bearing for the central claim of providing full 2→3 kinematics; the framework remains an extrapolation tool whose validity rests on the (explicitly flagged) assumption that the fitted amplitudes remain accurate in the target kinematic window. This is the standard structure of a data-driven phenomenological study and does not meet any of the enumerated circularity patterns.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

The central claim rests on the validity of data-constrained phenomenological amplitudes for the 2-to-3 process and on the assumption that forward-proton kinematics at EIC energies can be described by the same amplitudes used at lower energies.

pith-pipeline@v0.9.0 · 5522 in / 1152 out tokens · 41505 ms · 2026-05-10T16:51:40.224955+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

190 extracted references · 154 canonical work pages · 4 internal anchors

  1. [1]

    = ( ¯Q2 min, ¯Q2 max) and window : (Q 2 1, Q2

  2. [2]

    3 m2η −m 2a + 6 m2 η′ −m 2a + δI m2 π m2π −m 2a 1 m2η −m 2a + 2 m2 η′ −m 2a !# , gωγa(ma) ma<1.2 GeV = egm2 0 36π2fa

    = (1 GeV2, ¯Q2 max).(91) The second choice corresponds to the domain where the outgoing electron is typically within the range of the central EIC detectors. At the same time, it provides a direct test of the roughness of the approximation in Eq. (83), since it emphasizes the larger-Q 2 region where the factorized on-shell treatment is expected to become l...

  3. [3]

    Reduction to four invariants Following Ref. [184], we introduce the following set of kinematic invariants: s1 ≡(p e′ +p X)2 , s γ∗p ≡(p p′ +p X)2 = (pp +p e −p e′)2 , Q2 ≡ −(p e −p e′)2 , t p ≡(p p −p p′)2 .(C6) After integrating out the trivial angular variables, the phase-space measure reduces to dΦ3 = π 16 q λ(s, m2e, m2p) 4ds γ∗p dQ2 dtp ds1q λ(sγ∗p,−...

  4. [5]

    dressing

    Ensuring gauge invariance of the nucleon summand Let us discuss GI µ entering Eq. (D5) in more detail. To restore Ward identities, Refs. [103, 144] utilized the pole term GIµ =−γ 5(Gsγ∗ p − Gu) pγ∗,µ −Q2 , p γ∗ ≡p e −p e′,(D13) and then analyzed theγp→π 0pandγ ∗p→π 0pscatterings. However, we cannot use it for our calculations of the meson production in th...

  5. [6]

    Reconstructing energies and polar angles from invariants Given a sampled point (s 1, sγ∗p, Q2, tp), we reconstruct the event kinematics in theepc.m. frame. The final state energies follow from standard three-body kinematics: E∗ e′ = s+m 2 e −s γ∗p 2√s , p ∗ e′ = p λ(s, m2e, sγ∗p) 2√s , E∗ p′ = s+m 2 p −s 1 2√s , p ∗ p′ = q λ(s, m2p, s1) 2√s , E∗ X = s+m 2...

  6. [7]

    We sample this freedom by drawing one azimuth uniformly and determining the other two from transverse-momentum closure

    Azimuthal angles and full four-momenta The invariants fix all dot products among external momenta; in a collinear-beam setup, the remaining continuous freedom is a global rotation about the beam axis. We sample this freedom by drawing one azimuth uniformly and determining the other two from transverse-momentum closure. Define the transverse-momentum magni...

  7. [8]

    Electron Ion Collider: The Next QCD Frontier - Understanding the glue that binds us all

    A. Accardi et al.,Electron Ion Collider: The Next QCD Frontier: Understanding the glue that binds us all, Eur. Phys. J. A52(2016), no. 9 268, [arXiv:1212.1701]

  8. [9]

    Science Requirements and Detector Concepts for the Electron-Ion Collider: EIC Yellow Report

    R. Abdul Khalek et al.,Science Requirements and Detector Concepts for the Electron-Ion Collider: EIC Yellow Report,Nucl. Phys. A1026(2022) 122447, [arXiv:2103.05419]

  9. [10]

    Gonderinger and M

    M. Gonderinger and M. J. Ramsey-Musolf,Electron-to-Tau Lepton Flavor Violation at the Electron-Ion Collider,JHEP11(2010) 045, [arXiv:1006.5063]. [Erratum: JHEP 05, 047 (2012)]

  10. [11]

    Boughezal, F

    R. Boughezal, F. Petriello, and D. Wiegand,Removing flat directions in standard model EFT fits: How polarized electron-ion collider data can complement the LHC,Phys. Rev. D101(2020), no. 11 116002, [arXiv:2004.00748]

  11. [12]

    Liu and B

    Y. Liu and B. Yan,Searching for the axion-like particle at the EIC*,Chin. Phys. C47(2023), no. 4 043113, [arXiv:2112.02477]

  12. [13]

    Cirigliano, K

    V. Cirigliano, K. Fuyuto, C. Lee, E. Mereghetti, and B. Yan,Charged Lepton Flavor Violation at the EIC, JHEP03(2021) 256, [arXiv:2102.06176]

  13. [14]

    Davoudiasl, R

    H. Davoudiasl, R. Marcarelli, and E. T. Neil,Lepton-flavor-violating ALPs at the Electron-Ion Collider: a golden opportunity,JHEP02(2023) 071, [arXiv:2112.04513]

  14. [15]

    B. Yan, Z. Yu, and C. P. Yuan,The anomalous Zbb¯couplings at the HERA and EIC,Phys. Lett. B822 (2021) 136697, [arXiv:2107.02134]

  15. [16]

    H. T. Li, B. Yan, and C. P. Yuan,Jet charge: A new tool to probe the anomalous Zbb¯couplings at the EIC,Phys. Lett. B833(2022) 137300, [arXiv:2112.07747]

  16. [17]

    Batell, T

    B. Batell, T. Ghosh, T. Han, and K. Xie,Heavy neutral leptons at the Electron-Ion Collider,JHEP03 (2023) 020, [arXiv:2210.09287]

  17. [18]

    J. L. Zhang et al.,Search for e→τcharged lepton flavor violation at the EIC with the ECCE detector,Nucl. Instrum. Meth. A1053(2023) 168276, [arXiv:2207.10261]

  18. [19]

    Yan,Probing the dark photon via polarized DIS scattering at the HERA and EIC,Phys

    B. Yan,Probing the dark photon via polarized DIS scattering at the HERA and EIC,Phys. Lett. B833 (2022) 137384, [arXiv:2203.01510]

  19. [20]

    Boughezal, A

    R. Boughezal, A. Emmert, T. Kutz, S. Mantry, M. Nycz, F. Petriello, K. S ¸im¸ sek, D. Wiegand, and X. Zheng,Neutral-current electroweak physics and SMEFT studies at the EIC,Phys. Rev. D106(2022), no. 1 016006, [arXiv:2204.07557]

  20. [21]

    Davoudiasl, R

    H. Davoudiasl, R. Marcarelli, and E. T. Neil,Displaced signals of hidden vectors at the Electron-Ion Collider,Phys. Rev. D108(2023), no. 7 075017, [arXiv:2307.00102]

  21. [22]

    Balkin, O

    R. Balkin, O. Hen, W. Li, H. Liu, T. Ma, Y. Soreq, and M. Williams,Probing axion-like particles at the Electron-Ion Collider,JHEP02(2024) 123, [arXiv:2310.08827]

  22. [23]

    Davoudiasl, R

    H. Davoudiasl, R. Marcarelli, and E. T. Neil,Flavor-violating ALPs, electron g-2, and the Electron-Ion Collider,Phys. Rev. D109(2024), no. 11 115013, [arXiv:2402.17821]

  23. [24]

    Wang, X.-K

    H.-L. Wang, X.-K. Wen, H. Xing, and B. Yan,Probing the four-fermion operators via the transverse double spin asymmetry at the Electron-Ion Collider,Phys. Rev. D109(2024), no. 9 095025, [arXiv:2401.08419]

  24. [25]

    X.-K. Wen, B. Yan, Z. Yu, and C. P. Yuan,Dihadron azimuthal asymmetry and light-quark dipole moments at the Electron-Ion Collider,arXiv:2408.07255

  25. [26]

    Q. Gao, D. Lin, H. Liu, and T. Ma,Dark photons and axion-like particles at the electron-ion collider in China,JHEP06(2025) 070, [arXiv:2412.06301]

  26. [27]

    Du,Parity violation on longitudinal single-spin asymmetries at the EicC,Phys

    Y. Du,Parity violation on longitudinal single-spin asymmetries at the EicC,Phys. Rev. D111(2025), no. 11 116026, [arXiv:2412.20469]

  27. [28]

    Deng, X.-H

    Y. Deng, X.-H. Jiang, T. Liu, and B. Yan,Testing lepton flavor universality at the Electron-Ion Collider, JHEP06(2025) 157, [arXiv:2503.02605]

  28. [29]

    Davoudiasl and H

    H. Davoudiasl and H. Liu,Electron-ion collider as a discovery tool for invisible dark bosons,Phys. Rev. D 112(2025), no. 7 075001, [arXiv:2505.08871]

  29. [30]

    Bellafronte, S

    L. Bellafronte, S. Dawson, P. P. Giardino, and H. Liu,Probing Top Quark - Electron Interactions at Future Colliders,arXiv:2507.02039. 39

  30. [31]

    Jiang, Y

    X.-H. Jiang, Y. Liu, and B. Yan,Probing top-quark electroweak couplings indirectly at the Electron-Ion Collider,arXiv:2507.21477

  31. [32]

    Nucleon Energy Correlators as a Probe of Light-Quark Dipole Operators at the Electron-Ion Collider

    Y. Huang, X.-B. Tong, and H.-L. Wang,Nucleon energy correlators as a probe of light-quark dipole operators at the EIC,arXiv:2508.08516

  32. [33]

    Bar-Shalom and J

    S. Bar-Shalom and J. Wudka,Flavor physics at the EIC with b-jet tagging,arXiv:2601.03345

  33. [34]

    Adhikary, D

    A. Adhikary, D. K. Ghosh, S. Jeesun, and S. Roy,ALP andZ ′ boson at the Electron-Ion collider, arXiv:2601.04962

  34. [35]

    Urrutia Quiroga, V

    S. Urrutia Quiroga, V. Cirigliano, W. Dekens, K. Fuyuto, and E. Mereghetti,Flavorful Lepton Number Violation at the EIC,arXiv:2602.22355

  35. [36]

    Basso, A

    L. Basso, A. Belyaev, S. Moretti, and C. H. Shepherd-Themistocleous,Phenomenology of the minimal B-L extension of the Standard model: Z’ and neutrinos,Phys. Rev. D80(2009) 055030, [arXiv:0812.4313]

  36. [37]

    L. B. Okun,LIMITS OF ELECTRODYNAMICS: PARAPHOTONS?,Sov. Phys. JETP56(1982) 502

  37. [38]

    Holdom,Two U(1)’s and Epsilon Charge Shifts,Phys

    B. Holdom,Two U(1)’s and Epsilon Charge Shifts,Phys. Lett. B166(1986) 196–198

  38. [39]

    Heeck,Unbroken B – L symmetry,Phys

    J. Heeck,Unbroken B – L symmetry,Phys. Lett. B739(2014) 256–262, [arXiv:1408.6845]

  39. [40]

    Working Group Report: New Light Weakly Coupled Particles,

    R. Essig et al.,Working Group Report: New Light Weakly Coupled Particles, inSnowmass 2013: Snowmass on the Mississippi, 10, 2013.arXiv:1311.0029

  40. [41]

    Beachamet al., J

    J. Beacham et al.,Physics Beyond Colliders at CERN: Beyond the Standard Model Working Group Report, J. Phys. G47(2020), no. 1 010501, [arXiv:1901.09966]

  41. [42]

    Serendipity in dark photon searches

    P. Ilten, Y. Soreq, M. Williams, and W. Xue,Serendipity in dark photon searches,JHEP06(2018) 004, [arXiv:1801.04847]

  42. [43]

    Kyselov and M

    Y. Kyselov and M. Ovchynnikov,Searches for long-lived dark photons at proton accelerator experiments, Phys. Rev. D111(2025), no. 1 015030, [arXiv:2409.11096]

  43. [44]

    Dimopoulos,A Solution of the Strong CP Problem in Models With Scalars,Phys

    S. Dimopoulos,A Solution of the Strong CP Problem in Models With Scalars,Phys. Lett. B84(1979) 435–439

  44. [45]

    Holdom and M

    B. Holdom and M. E. Peskin,Raising the Axion Mass,Nucl. Phys. B208(1982) 397–412

  45. [46]

    J. M. Flynn and L. Randall,A Computation of the Small Instanton Contribution to the Axion Potential, Nucl. Phys. B293(1987) 731–739

  46. [47]

    V. A. Rubakov,Grand unification and heavy axion,JETP Lett.65(1997) 621–624, [hep-ph/9703409]

  47. [48]

    Berezhiani, L

    Z. Berezhiani, L. Gianfagna, and M. Giannotti,Strong CP problem and mirror world: The Weinberg-Wilczek axion revisited,Phys. Lett. B500(2001) 286–296, [hep-ph/0009290]

  48. [49]

    Fukuda, K

    H. Fukuda, K. Harigaya, M. Ibe, and T. T. Yanagida,Model of visible QCD axion,Phys. Rev. D92(2015), no. 1 015021, [arXiv:1504.06084]

  49. [50]

    Gherghetta, N

    T. Gherghetta, N. Nagata, and M. Shifman,A Visible QCD Axion from an Enlarged Color Group,Phys. Rev. D93(2016), no. 11 115010, [arXiv:1604.01127]

  50. [51]

    Dimopoulos, A

    S. Dimopoulos, A. Hook, J. Huang, and G. Marques-Tavares,A collider observable QCD axion,JHEP11 (2016) 052, [arXiv:1606.03097]

  51. [52]

    Fukuda, M

    H. Fukuda, M. Ibe, and T. T. Yanagida,Dark Matter Candidates in a Visible Heavy QCD Axion Model, Phys. Rev. D95(2017), no. 9 095017, [arXiv:1702.00227]

  52. [53]

    Agrawal and K

    P. Agrawal and K. Howe,Factoring the Strong CP Problem,JHEP12(2018) 029, [arXiv:1710.04213]

  53. [54]

    M. K. Gaillard, M. B. Gavela, R. Houtz, P. Quilez, and R. Del Rey,Color unified dynamical axion,Eur. Phys. J. C78(2018), no. 11 972, [arXiv:1805.06465]

  54. [55]

    Lillard and T.M.P

    B. Lillard and T. M. P. Tait,A High Quality Composite Axion,JHEP11(2018) 199, [arXiv:1811.03089]

  55. [56]

    A. Hook, S. Kumar, Z. Liu, and R. Sundrum,High Quality QCD Axion and the LHC,Phys. Rev. Lett.124 (2020), no. 22 221801, [arXiv:1911.12364]

  56. [57]

    Cs´ aki, M

    C. Cs´ aki, M. Ruhdorfer, and Y. Shirman,UV Sensitivity of the Axion Mass from Instantons in Partially Broken Gauge Groups,JHEP04(2020) 031, [arXiv:1912.02197]

  57. [58]

    Gherghetta, V.V

    T. Gherghetta, V. V. Khoze, A. Pomarol, and Y. Shirman,The Axion Mass from 5D Small Instantons, JHEP03(2020) 063, [arXiv:2001.05610]

  58. [59]

    Valenti, L

    A. Valenti, L. Vecchi, and L.-X. Xu,Grand Color axion,JHEP10(2022) 025, [arXiv:2206.04077]

  59. [60]

    Kivel, J

    A. Kivel, J. Laux, and F. Yu,Supersizing axions with small size instantons,JHEP11(2022) 088, [arXiv:2207.08740]

  60. [61]

    D. I. Dunsky, L. J. Hall, and K. Harigaya,A heavy QCD axion and the mirror world,JHEP02(2024) 212, [arXiv:2302.04274]

  61. [62]

    M. J. Dolan, T. Ferber, C. Hearty, F. Kahlhoefer, and K. Schmidt-Hoberg,Revised constraints and Belle II sensitivity for visible and invisible axion-like particles,JHEP12(2017) 094, [arXiv:1709.00009]. [Erratum: JHEP 03, 190 (2021)]

  62. [63]

    D. S. M. Alves and N. Weiner,A viable QCD axion in the MeV mass range,JHEP07(2018) 092, [arXiv:1710.03764]

  63. [64]

    W. J. Marciano, A. Masiero, P. Paradisi, and M. Passera,Contributions of axionlike particles to lepton dipole moments,Phys. Rev. D94(2016), no. 11 115033, [arXiv:1607.01022]

  64. [65]

    Probing MeV to 90 GeV axion-like particles with LEP and LHC,

    J. Jaeckel and M. Spannowsky,Probing MeV to 90 GeV axion-like particles with LEP and LHC,Phys. Lett. B753(2016) 482–487, [arXiv:1509.00476]

  65. [66]

    ALPtraum: ALP production in proton beam dump experiments,

    B. D¨ obrich, J. Jaeckel, F. Kahlhoefer, A. Ringwald, and K. Schmidt-Hoberg,ALPtraum: ALP production in proton beam dump experiments,JHEP02(2016) 018, [arXiv:1512.03069]. 40

  66. [67]

    Izaguirre, T

    E. Izaguirre, T. Lin, and B. Shuve,Searching for Axionlike Particles in Flavor-Changing Neutral Current Processes,Phys. Rev. Lett.118(2017), no. 11 111802, [arXiv:1611.09355]

  67. [68]

    Searching for Axionlike Particles with Ultraperipheral Heavy-Ion Collisions,

    S. Knapen, T. Lin, H. K. Lou, and T. Melia,Searching for Axionlike Particles with Ultraperipheral Heavy-Ion Collisions,Phys. Rev. Lett.118(2017), no. 17 171801, [arXiv:1607.06083]

  68. [69]

    Bauer, M

    M. Bauer, M. Heiles, M. Neubert, and A. Thamm,Axion-Like Particles at Future Colliders,Eur. Phys. J. C79(2019), no. 1 74, [arXiv:1808.10323]

  69. [70]

    Mariotti, D

    A. Mariotti, D. Redigolo, F. Sala, and K. Tobioka,New LHC bound on low-mass diphoton resonances,Phys. Lett. B783(2018) 13–18, [arXiv:1710.01743]

  70. [71]

    Cid Vidal, A

    X. Cid Vidal, A. Mariotti, D. Redigolo, F. Sala, and K. Tobioka,New Axion Searches at Flavor Factories, JHEP01(2019) 113, [arXiv:1810.09452]. [Erratum: JHEP 06, 141 (2020)]

  71. [72]

    Aloni, Y

    D. Aloni, Y. Soreq, and M. Williams,Coupling QCD-Scale Axionlike Particles to Gluons,Phys. Rev. Lett. 123(2019), no. 3 031803, [arXiv:1811.03474]

  72. [73]

    Aloni, C

    D. Aloni, C. Fanelli, Y. Soreq, and M. Williams,Photoproduction of Axionlike Particles,Phys. Rev. Lett. 123(2019), no. 7 071801, [arXiv:1903.03586]

  73. [74]

    Bauer, M

    M. Bauer, M. Neubert, S. Renner, M. Schnubel, and A. Thamm,The Low-Energy Effective Theory of Axions and ALPs,JHEP04(2021) 063, [arXiv:2012.12272]

  74. [75]

    Bauer, M

    M. Bauer, M. Neubert, S. Renner, M. Schnubel, and A. Thamm,Consistent Treatment of Axions in the Weak Chiral Lagrangian,Phys. Rev. Lett.127(2021), no. 8 081803, [arXiv:2102.13112]

  75. [76]

    Sakaki and D

    Y. Sakaki and D. Ueda,Searching for new light particles at the international linear collider main beam dump,Phys. Rev. D103(2021), no. 3 035024, [arXiv:2009.13790]

  76. [77]

    Fl´ orez, A

    A. Fl´ orez, A. Gurrola, W. Johns, P. Sheldon, E. Sheridan, K. Sinha, and B. Soubasis,Probing axionlike particles withγγfinal states from vector boson fusion processes at the LHC,Phys. Rev. D103(2021), no. 9 095001, [arXiv:2101.11119]

  77. [78]

    Brdar, B

    V. Brdar, B. Dutta, W. Jang, D. Kim, I. M. Shoemaker, Z. Tabrizi, A. Thompson, and J. Yu,Axionlike Particles at Future Neutrino Experiments: Closing the Cosmological Triangle,Phys. Rev. Lett.126(2021), no. 20 201801, [arXiv:2011.07054]

  78. [79]

    Bertholet, S

    E. Bertholet, S. Chakraborty, V. Loladze, T. Okui, A. Soffer, and K. Tobioka,Heavy QCD axion at Belle II: Displaced and prompt signals,Phys. Rev. D105(2022), no. 7 L071701, [arXiv:2108.10331]

  79. [80]

    R. T. Co, S. Kumar, and Z. Liu,Searches for heavy QCD axions via dimuon final states,JHEP02(2023) 111, [arXiv:2210.02462]

  80. [81]

    Trifinopoulos and M

    S. Trifinopoulos and M. Vanvlasselaer,Attracting the electroweak scale to a tachyonic trap,Phys. Rev. D 107(2023), no. 7 L071701, [arXiv:2210.13484]

Showing first 80 references.