Recognition: 2 theorem links
· Lean TheoremBraking protons at the EIC: from invisible meson decay to new physics searches
Pith reviewed 2026-05-16 17:56 UTC · model grok-4.3
The pith
The Electron-Ion Collider can improve bounds on invisible pseudoscalar meson decays by up to four orders of magnitude.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In coherent exclusive electroproduction at the EIC a forward proton with reduced energy and minimal additional activity tags invisible final states. For pseudoscalar mesons this allows branching-ratio sensitivities as low as 10^{-8} for eta and eta-prime invisible decays, strengthening current bounds by up to four orders of magnitude. The same channel directly constrains gluon-coupled ALPs that decay invisibly, reaching decay constants up to 10^5 GeV for masses between 0.1 and 2 GeV.
What carries the argument
Forward proton with reduced energy in coherent exclusive electroproduction, which tags invisible final states while kinematics and particle detection suppress backgrounds.
If this is right
- New upper limits would be set on invisible branching ratios of the neutral pion, eta, and eta-prime mesons.
- ALPs with gluon couplings and fa up to 10^5 GeV would be excluded or discovered in the 0.1-2 GeV mass range.
- The same experimental signature applies to other invisible final states beyond the cases explicitly studied.
- Kinematic tagging of the forward proton becomes a standard tool for invisible searches at electron-ion facilities.
Where Pith is reading between the lines
- If the background suppression holds, analogous forward-proton tagging could be tested at other high-energy electron facilities.
- Tighter meson decay bounds would indirectly constrain hidden-sector models that couple to Standard Model pseudoscalars.
- ALP limits in this mass window would complement existing beam-dump and collider searches by covering a different coupling regime.
Load-bearing premise
Backgrounds from other processes can be reduced far below the signal rate by using the EIC's particle detection and kinematics reconstruction.
What would settle it
A calculation or measurement showing that irreducible backgrounds remain above the level needed to reach branching ratios of 10^{-8} would falsify the projected sensitivity.
Figures
read the original abstract
We investigate the sensitivity of the Electron-Ion Collider (EIC) to invisible final states in coherent exclusive electroproduction. The characteristic signal is a forward proton with reduced energy and little additional detector activity. Using the excellent particle detection capabilities and kinematics reconstruction at the EIC, we argue that backgrounds can be strongly suppressed. While our analysis applies to various states, we specifically focus on pseudoscalar particles: (i) neutral mesons ($\pi^0,\eta^{(\prime)}$), whose invisible Standard Model decays are extremely suppressed, and (ii) gluon-coupled axion-like particles (ALPs) decaying invisibly to a dark sector. Depending on the meson species and the achievable background rejection, the EIC could strengthen existing bounds on invisible decays of pseudoscalar mesons by up to four orders of magnitude, probing branching ratios as small as ${\rm BR}(\eta^{(\prime)}\to{\rm inv})\sim 10^{-8}$. In addition, the EIC would directly probe invisibly decaying ALPs with the couplings up to $f_a\sim 10^5\,\text{GeV}$ and masses in the range $0.1$-$2\,\text{GeV}$.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript investigates the sensitivity of the Electron-Ion Collider (EIC) to invisible final states in coherent exclusive electroproduction. The signal is characterized by a forward proton with reduced energy and minimal additional detector activity. Focusing on pseudoscalar mesons (π⁰, η, η') with invisible Standard Model decays and gluon-coupled axion-like particles (ALPs) decaying invisibly to a dark sector, the authors argue that EIC particle detection and kinematics reconstruction enable strong background suppression. This would allow probing branching ratios as small as BR(η(')→inv)∼10^{-8}, strengthening existing bounds by up to four orders of magnitude, and directly constraining invisibly decaying ALPs with f_a up to ∼10^5 GeV for masses 0.1-2 GeV.
Significance. If the background suppression assumptions hold, the work would provide a novel probe of rare invisible meson decays and ALP couplings in a mass range complementary to existing experiments, potentially improving limits by several orders of magnitude using the EIC's unique kinematics.
major comments (1)
- [Abstract] Abstract and background discussion: the central claims of four-order improvement in BR(η(')→inv) sensitivity to ∼10^{-8} and ALP reach to f_a∼10^5 GeV rest on the assertion that backgrounds (single-diffractive dissociation, beam remnants, mis-tagged elastic scattering, photon-induced processes) can be strongly suppressed. However, no quantitative rejection factors, residual background rates after cuts, efficiency curves versus Q²/x, or simulation details are supplied, rendering the projections extrapolations rather than calculated results.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive feedback. The major comment correctly identifies that the sensitivity projections rest on background-suppression arguments without accompanying quantitative details. We address this below and will revise the manuscript accordingly.
read point-by-point responses
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Referee: [Abstract] Abstract and background discussion: the central claims of four-order improvement in BR(η(')→inv) sensitivity to ∼10^{-8} and ALP reach to f_a∼10^5 GeV rest on the assertion that backgrounds (single-diffractive dissociation, beam remnants, mis-tagged elastic scattering, photon-induced processes) can be strongly suppressed. However, no quantitative rejection factors, residual background rates after cuts, efficiency curves versus Q²/x, or simulation details are supplied, rendering the projections extrapolations rather than calculated results.
Authors: We agree that the current manuscript presents the projected sensitivities based on qualitative arguments for background rejection rather than explicit quantitative simulations. In the revised version we will add a dedicated section containing Monte Carlo studies of the listed backgrounds. These will include (i) rejection factors achieved by the forward-proton tagging and veto requirements, (ii) residual background rates after all cuts, and (iii) efficiency curves versus Q² and x. The updated projections will then be derived from these calculated quantities rather than from the existing extrapolations. revision: yes
Circularity Check
No significant circularity; sensitivity projections rely on external detector assumptions
full rationale
The paper presents projected EIC reach for invisible meson decays and ALPs based on assumed background suppression from detector performance and kinematics reconstruction. No equations reduce the claimed BR~10^{-8} or fa~10^5 GeV contours to fitted parameters defined by the same data. No self-definitional steps, fitted inputs renamed as predictions, or load-bearing self-citations appear in the derivation chain. The analysis is self-contained against external benchmarks of EIC capabilities, with the central claim resting on unverified but independent assumptions rather than tautological reduction.
Axiom & Free-Parameter Ledger
free parameters (1)
- background rejection efficiency
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Using the excellent particle detection capabilities and kinematics reconstruction at the EIC, we argue that backgrounds can be strongly suppressed... probing branching ratios as small as BR(η(')→inv)∼10^{-8}
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
The characteristic signal is a forward proton with reduced energy and little additional detector activity
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Forward citations
Cited by 1 Pith paper
-
On Exclusive Coherent Production of Bosons in Electron-Proton Collisions
A phenomenological 2-to-3 framework is constructed for exclusive boson electroproduction that matches flux-factorized predictions near Q^{2}=0 while capturing finite-Q^{2} effects at larger virtualities.
Reference graph
Works this paper leans on
-
[1]
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]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[2]
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]
work page internal anchor Pith review Pith/arXiv arXiv 2022
-
[3]
Electron-to-Tau Lepton Flavor Violation at the Electron-Ion Collider
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)]
work page internal anchor Pith review Pith/arXiv arXiv 2010
-
[4]
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]
- [5]
-
[6]
V. Cirigliano, K. Fuyuto, C. Lee, E. Mereghetti, and B. Yan,Charged Lepton Flavor Violation at the EIC, JHEP03(2021) 256, [arXiv:2102.06176]
-
[7]
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]
- [8]
- [9]
- [10]
- [11]
-
[12]
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]
-
[13]
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]
-
[14]
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]
- [15]
-
[16]
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]
-
[17]
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]
- [18]
- [19]
-
[20]
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]
-
[21]
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]
-
[22]
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]
-
[23]
L. Bellafronte, S. Dawson, P. P. Giardino, and H. Liu, Probing Top Quark - Electron Interactions at Future Colliders,arXiv:2507.02039
- [24]
-
[25]
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
work page internal anchor Pith review Pith/arXiv arXiv
-
[26]
A. Jentsch,Physics Opportunities in the Far-forward Region at the Future Electron–Ion Collider,Acta Phys. Pol. B Proc. Suppl.16(2023) 7–A13
work page 2023
-
[27]
M. Pitt,Physics Perspectives with the ePIC Far-Forward and Far-Backward detectors,PoS DIS2024(2025) 259, [arXiv:2409.02811]
-
[28]
Note on invisible decays of light mesons
D.-N. Gao,Note on invisible decays of light mesons, Phys. Rev. D98(2018), no. 11 113006, [arXiv:1811.10152]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[29]
Constraints on Light Dark Matter and U bosons, from psi, Upsilon, K+, pi0, eta and eta' decays
P. Fayet,Constraints on Light Dark Matter and U bosons, from psi, Upsilon, K+, pi0, eta and eta-prime decays,Phys. Rev. D74(2006) 054034, [hep-ph/0607318]
work page internal anchor Pith review Pith/arXiv arXiv 2006
-
[30]
J. F. Kamenik and C. Smith,FCNC portals to the dark sector,JHEP03(2012) 090, [arXiv:1111.6402]
work page internal anchor Pith review Pith/arXiv arXiv 2012
-
[31]
S. N. Gninenko,Search for invisible decays of π0, η, η′, KS andK L: A probe of new physics and tests using the Bell-Steinberger relation,Phys. Rev. D91 (2015), no. 1 015004, [arXiv:1409.2288]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[32]
S. N. Gninenko and N. V. Krasnikov,InvisibleK L 7 decays as a probe of new physics,Phys. Rev. D92 (2015), no. 3 034009, [arXiv:1503.01595]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[33]
S. N. Gninenko and N. V. Krasnikov,InvisibleK L decays in the SM extensions,Mod. Phys. Lett. A31 (2016), no. 25 1650142, [arXiv:1602.03548]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[34]
Neutral Hadrons Disappearing into the Darkness
D. Barducci, M. Fabbrichesi, and E. Gabrielli,Neutral Hadrons Disappearing into the Darkness,Phys. Rev. D 98(2018), no. 3 035049, [arXiv:1806.05678]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[35]
M. Hostert, K. Kaneta, and M. Pospelov,Pair production of dark particles in meson decays,Phys. Rev. D102(2020), no. 5 055016, [arXiv:2005.07102]. [36]REDTOPCollaboration, J. Elam et al.,The REDTOP experiment: Rareη/η ′ Decays To Probe New Physics,arXiv:2203.07651
- [36]
-
[37]
Invisible Quarkonium Decays as a Sensitive Probe of Dark Matter
B. McElrath,Invisible quarkonium decays as a sensitive probe of dark matter,Phys. Rev. D72(2005) 103508, [hep-ph/0506151]
work page internal anchor Pith review Pith/arXiv arXiv 2005
-
[38]
Leptophobic Dark Matter at Neutrino Factories
B. Batell, P. deNiverville, D. McKeen, M. Pospelov, and A. Ritz,Leptophobic Dark Matter at Neutrino Factories,Phys. Rev. D90(2014), no. 11 115014, [arXiv:1405.7049]
work page internal anchor Pith review Pith/arXiv arXiv 2014
- [39]
-
[40]
L. Darm´ e, S. A. R. Ellis, and T. You,Light Dark Sectors through the Fermion Portal,JHEP07(2020) 053, [arXiv:2001.01490]
-
[41]
Y. Ema, F. Sala, and R. Sato,Neutrino experiments probe hadrophilic light dark matter,SciPost Phys.10 (2021), no. 3 072, [arXiv:2011.01939]. [43]NA62Collaboration, E. Cortina Gil et al.,Search for π0 decays to invisible particles,JHEP02(2021) 201, [arXiv:2010.07644]. [44]NA64Collaboration, Y. M. Andreev et al., Dark-Sector Search via Pion-Producedηandη’ M...
-
[42]
R. D. Peccei and H. R. Quinn,CP Conservation in the Presence of Instantons,Phys. Rev. Lett.38(1977) 1440–1443
work page 1977
-
[43]
R. D. Peccei and H. R. Quinn,Constraints Imposed by CP Conservation in the Presence of Instantons,Phys. Rev. D16(1977) 1791–1797
work page 1977
-
[44]
Weinberg,A New Light Boson?,Phys
S. Weinberg,A New Light Boson?,Phys. Rev. Lett.40 (1978) 223–226
work page 1978
-
[45]
Wilczek,Problem of StrongPandTInvariance in the Presence of Instantons,Phys
F. Wilczek,Problem of StrongPandTInvariance in the Presence of Instantons,Phys. Rev. Lett.40(1978) 279–282
work page 1978
-
[46]
L. F. Abbott and P. Sikivie,A Cosmological Bound on the Invisible Axion,Phys. Lett. B120(1983) 133–136
work page 1983
-
[47]
M. Dine and W. Fischler,The Not So Harmless Axion, Phys. Lett. B120(1983) 137–141
work page 1983
-
[48]
J. Preskill, M. B. Wise, and F. Wilczek,Cosmology of the Invisible Axion,Phys. Lett. B120(1983) 127–132
work page 1983
-
[49]
D. J. E. Marsh,Axion Cosmology,Phys. Rept.643 (2016) 1–79, [arXiv:1510.07633]
work page internal anchor Pith review Pith/arXiv arXiv 2016
- [50]
-
[51]
Dark Matter through the Axion Portal
Y. Nomura and J. Thaler,Dark Matter through the Axion Portal,Phys. Rev. D79(2009) 075008, [arXiv:0810.5397]
work page internal anchor Pith review Pith/arXiv arXiv 2009
-
[52]
On dark matter models with uniquely spin-dependent detection possibilities
M. Freytsis and Z. Ligeti,On dark matter models with uniquely spin-dependent detection possibilities,Phys. Rev. D83(2011) 115009, [arXiv:1012.5317]
work page internal anchor Pith review Pith/arXiv arXiv 2011
-
[53]
M. J. Dolan, F. Kahlhoefer, C. McCabe, and K. Schmidt-Hoberg,A taste of dark matter: Flavour constraints on pseudoscalar mediators,JHEP03 (2015) 171, [arXiv:1412.5174]. [Erratum: JHEP 07, 103 (2015)]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[54]
SIMPs through the axion portal
Y. Hochberg, E. Kuflik, R. Mcgehee, H. Murayama, and K. Schutz,Strongly interacting massive particles through the axion portal,Phys. Rev. D98(2018), no. 11 115031, [arXiv:1806.10139]
work page internal anchor Pith review Pith/arXiv arXiv 2018
- [55]
- [56]
- [57]
-
[58]
The epic detector and collaboration
ePIC Collaboration, “The epic detector and collaboration.”https://www.bnl.gov/eic/epic.php, 2025
work page 2025
-
[59]
V. Burkert et al.,Precision studies of qcd in the low energy domain of the eic,Progress in Particle and Nuclear Physics131(2023) 104032
work page 2023
-
[60]
Nadel-Turonski,A Second Detector for the Electron-Ion Collider,PoSDIS2024(2024) 283
P. Nadel-Turonski,A Second Detector for the Electron-Ion Collider,PoSDIS2024(2024) 283
work page 2024
-
[61]
E. C. Aschenauer, A. Bazilevsky, A. Jentsch, J. Kim, A. Kiselev, B. S. Page, Z. Tu, T. Ullrich, and C. P. Wong,Tagging efficiency study of incoherent diffractive vector meson production at the second interaction region at the electron-ion collider,Phys. Rev. D111(Apr, 2025) 072013
work page 2025
-
[62]
Allaire et al.,Artificial Intelligence for the Electron Ion Collider (AI4EIC),Comput
C. Allaire et al.,Artificial Intelligence for the Electron Ion Collider (AI4EIC),Comput. Softw. Big Sci.8 (2024) 5, [arXiv:2307.08593]
- [63]
-
[64]
A. Jentsch, Z. Tu, and C. Weiss,Deep-inelastic electron-deuteron scattering with spectator nucleon tagging at the future electron ion collider: Extracting free nucleon structure,Phys. Rev. C104(Dec, 2021) 065205
work page 2021
-
[65]
E. C. Aschenauer, V. Batozskaya, S. Fazio, A. Jentsch, J. Kim, K. Kumeriˇ cki, H. Moutarde, K. Passek-K., D. Sokhan, H. Spiesberger, P. Sznajder, and K. Tezgin, Study of deeply virtual compton scattering at the future electron-ion collider,Phys. Rev. D112(Aug, 2025) 036010
work page 2025
-
[66]
Planck-Scale Physics and the Peccei-Quinn Mechanism
M. Kamionkowski and J. March-Russell,Planck scale physics and the Peccei-Quinn mechanism,Phys. Lett. B282(1992) 137–141, [hep-th/9202003]
work page internal anchor Pith review Pith/arXiv arXiv 1992
-
[67]
Solutions to the strong CP problem in a world with gravity
R. Holman, S. D. H. Hsu, T. W. Kephart, E. W. Kolb, R. Watkins, and L. M. Widrow,Solutions to the strong CP problem in a world with gravity,Phys. Lett. B282 (1992) 132–136, [hep-ph/9203206]. 8
work page internal anchor Pith review Pith/arXiv arXiv 1992
-
[68]
S. M. Barr and D. Seckel,Planck scale corrections to axion models,Phys. Rev. D46(1992) 539–549
work page 1992
- [69]
-
[70]
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
work page 1979
-
[71]
B. Holdom and M. E. Peskin,Raising the Axion Mass, Nucl. Phys. B208(1982) 397–412
work page 1982
-
[72]
J. M. Flynn and L. Randall,A Computation of the Small Instanton Contribution to the Axion Potential, Nucl. Phys. B293(1987) 731–739
work page 1987
-
[73]
V. A. Rubakov,Grand unification and heavy axion, JETP Lett.65(1997) 621–624, [hep-ph/9703409]
work page internal anchor Pith review Pith/arXiv arXiv 1997
-
[74]
Strong CP problem and mirror world: the Weinberg Wilczek axion revisited
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]
work page internal anchor Pith review Pith/arXiv arXiv 2001
-
[75]
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]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[76]
A Visible QCD Axion from an Enlarged Color Group
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]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[77]
A collider observable QCD axion
S. Dimopoulos, A. Hook, J. Huang, and G. Marques-Tavares,A collider observable QCD axion, JHEP11(2016) 052, [arXiv:1606.03097]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[78]
Dark Matter Candidates in a Visible Heavy QCD Axion Model
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]
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[79]
Factoring the Strong CP Problem
P. Agrawal and K. Howe,Factoring the Strong CP Problem,JHEP12(2018) 029, [arXiv:1710.04213]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[80]
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]
work page internal anchor Pith review Pith/arXiv arXiv 2018
discussion (0)
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