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arxiv: 2512.01638 · v2 · submitted 2025-12-01 · 🌌 astro-ph.GA · astro-ph.HE· astro-ph.IM· hep-ex

Recognition: 1 theorem link

Searching for EeV photons with Telescope Array Surface Detector and neural networks

Telescope Array Collaboration: R.U. Abbasi , T. Abu-Zayyad , M. Allen , J.W. Belz , D.R. Bergman , F. Bradfield , I. Buckland , W. Campbell
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B.G. Cheon K. Endo A. Fedynitch T. Fujii K. Fujisue K. Fujita (5) M. Fukushima (5) G. Furlich (2) A. Galvez Urena (8) Z. Gerber (2) N. Globus (9) T. Hanaoka (10) W. Hanlon (2) N. Hayashida (11) H. He (12) K. Hibino (11) R. Higuchi (12) D. Ikeda (11) D. Ivanov (2) S. Jeong (13) C.C.H. Jui (2) K. Kadota (14) F. Kakimoto (11) O. Kalashev (15) K. Kasahara (16) Y. Kawachi (3) K. Kawata (5) I. Kharuk (15) E. Kido (5) H.B. Kim (4) J.H. Kim (2) S.W. Kim (13) R. Kobo (3) I. Komae (3) K. Komatsu (17) K. Komori (10) A. Korochkin (18) C. Koyama (5) M. Kudenko (15) M. Kuroiwa (17) Y. Kusumori (10) M. Kuznetsov (15) Y.J. Kwon (19) K.H. Lee (4) M.J. Lee (13) B. Lubsandorzhiev (15) J.P. Lundquist (2 20) H. Matsushita (3) A. Matsuzawa (17) J.A. Matthews (2) J.N. Matthews (2) K. Mizuno (17) M. Mori (10) S. Nagataki (12) K. Nakagawa (3) M. Nakahara (3) H. Nakamura (10) T. Nakamura (21) T. Nakayama (17) Y. Nakayama (10) K. Nakazawa (10) T. Nonaka (5) S. Ogio (5) H. Ohoka (5) N. Okazaki (5) M. Onishi (5) A. Oshima (22) H. Oshima (5) S. Ozawa (23) I.H. Park (13) K.Y. Park (4) M. Potts (2) M. Przybylak (24) M.S. Pshirkov (15 25) J. Remington (2) C. Rott (2) G.I. Rubtsov (15) D. Ryu (26) H. Sagawa (5) N. Sakaki (5) R. Sakamoto (10) T. Sako (5) N. Sakurai (5) S. Sakurai (3) D. Sato (17) K. Sekino (5) T. Shibata (5) J. Shikita (3) H. Shimodaira (5) H.S. Shin (3 7) K. Shinozaki (27) J.D. Smith (2) P. Sokolsky (2) B.T. Stokes (2) T.A. Stroman (2) H. Tachibana (3) K. Takahashi (5) M. Takeda (5) R. Takeishi (5) A. Taketa (28) M. Takita (5) Y. Tameda (10) K. Tanaka (29) M. Tanaka (30) M. Teramoto (10) S.B. Thomas (2) G.B. Thomson (2) P. Tinyakov (15 18) I. Tkachev (15) T. Tomida (17) S. Troitsky (15) Y. Tsunesada (3 S. Udo (11) F.R. Urban (8) M. Vrabel (27) D. Warren (12) K. Yamazaki (22) Y. Zhezher (5 15) Z. Zundel (2) J. Zvirzdin (2) ((1) Department of Physics Loyola University-Chicago Chicago Illinois 60660 USA (2) High Energy Astrophysics Institute Department of Physics Astronomy University of Utah Salt Lake City Utah 84112-0830 (3) Graduate School of Science Osaka Metropolitan University Sugimoto Sumiyoshi Osaka 558-8585 Japan (4) Department of Physics The Research Institute of Natural Science Hanyang University Seongdong-gu Seoul 426-791 Korea (5) Institute for Cosmic Ray Research University of Tokyo Kashiwa Chiba 277-8582 (6) Institute of Physics Academia Sinica Taipei City 115201 Taiwan (7) Nambu Yoichiro Institute of Theoretical Experimental Physics (8) CEICO Institute of Physics Czech Academy of Sciences Prague 182 21 Czech Republic (9) Institute of Astronomy National Autonomous University of Mexico Ensenada Campus Ensenada BC 22860 Mexico (10) Graduate School of Engineering Osaka Electro-Communication University Neyagawa-shi Osaka 572-8530 (11) Faculty of Engineering Kanagawa University Yokohama Kanagawa 221-8686 (12) Astrophysical Big Bang Laboratory RIKEN Wako Saitama 351-0198 (13) Department of Physics Sungkyunkwan University Jang-an-gu Suwon 16419 (14) Department of Physics Tokyo City University Setagaya-ku Tokyo 158-8557 (15) Institute for Nuclear Research of the Russian Academy of Sciences Moscow 117312 Russia (16) Faculty of Systems Engineering Science Shibaura Institute of Technology Minumaku Tokyo 337-8570 (17) Academic Assembly School of Science Technology Institute of Engineering Shinshu University Nagano Nagano 380-8554 (18) Service de Physique Theorique Universite Libre de Bruxelles Brussels 1050 Belgium (19) Department of Physics Yonsei University Seodaemun-gu Seoul 120-749 (20) Center for Astrophysics Cosmology University of Nova Gorica Nova Gorica 5297 Slovenia (21) Faculty of Science Kochi University Kochi Kochi 780-8520 (22) College of Science Engineering Chubu University Kasugai Aichi 487-8501 (23) Quantum ICT Advanced Development Center National Institute for Information Communications Technology Koganei Tokyo 184-8795 (24) Doctoral School of Exact Natural Sciences University of Lodz Lodz Lodz 90-237 Poland (25) Sternberg Astronomical Institute Moscow M.V. Lomonosov State University Moscow 119991 (26) Department of Physics School of Natural Sciences Ulsan National Institute of Science Technology UNIST-gil Ulsan 689-798 (27) Astrophysics Division National Centre for Nuclear Research Warsaw 02-093 (28) Earthquake Research Institute Bunkyo-ku Tokyo 277-8582 (29) Graduate School of Information Sciences Hiroshima City University Hiroshima Hiroshima 731-3194 (30) Institute of Particle Nuclear Studies KEK Tsukuba Ibaraki 305-0801 Japan)
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Pith reviewed 2026-05-17 03:23 UTC · model grok-4.3

classification 🌌 astro-ph.GA astro-ph.HEastro-ph.IMhep-ex
keywords ultra-high-energy photonsTelescope Arrayneural networkscosmic ray compositionphoton flux limitssurface detectorhadronic backgroundair showers
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The pith

Neural network analysis of Telescope Array data finds photon candidates consistent with hadronic background and sets new upper limits on ultra-high-energy photon flux.

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

The paper uses a neural network to separate photon-induced from proton-induced air showers in 14 years of data from the Telescope Array Surface Detector. Inputs combine reconstructed parameters sensitive to composition with raw time-resolved signals from the detector stations. Fine-tuning the network on a subset of real experimental data reduces reliance on Monte Carlo simulations that may not perfectly match observations. The resulting count of photon candidates matches the expected background from hadrons, allowing the derivation of upper limits on the diffuse photon flux above 10^19 eV and 10^20 eV.

Core claim

The analysis classifies events with a neural network trained on simulations and fine-tuned on experimental data, finding the number of photon candidates consistent with the expected hadronic background and yielding upper limits Φ_γ(E_γ > 10^19 eV) < 2.3 · 10^{-3} and Φ_γ(E_γ > 10^20 eV) < 3.0 · 10^{-4} (km² sr yr)^{-1}.

What carries the argument

Neural network classifier trained on Monte Carlo simulations of photon and proton showers and fine-tuned on a subset of real Surface Detector data to distinguish events using both composition parameters and raw signals.

If this is right

  • The limits constrain models of ultra-high-energy cosmic ray sources that predict substantial photon production.
  • The approach shows how neural networks can reduce simulation biases in composition analyses at the highest energies.
  • Continued operation of the Surface Detector will allow these flux limits to be tightened with increased exposure.
  • The method provides a template for similar searches at other ground-based cosmic ray arrays.

Where Pith is reading between the lines

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

  • The same fine-tuning strategy might improve photon-hadron separation in hybrid detector systems that combine surface and fluorescence measurements.
  • If no photons are found even with larger datasets, it would further disfavor certain beyond-Standard-Model scenarios that predict EeV photon fluxes.
  • Cross-checking the neural network output against independent composition estimators could test the robustness of the classification.

Load-bearing premise

The fine-tuned neural network correctly identifies photon events versus proton events without introducing bias from mismatches between simulations and actual data.

What would settle it

Detection of a statistically significant excess of photon-candidate events above the predicted hadronic background in the classified dataset would indicate a real photon flux and invalidate the upper limits.

read the original abstract

Ultra-high-energy photons play an important role in probing astrophysical models and beyond-Standard-Model scenarios. We report updated limits on the diffuse photon flux using Telescope Array's Surface Detector data collected over 14 years of operation. Our method employs a neural network classifier to effectively distinguish between proton-induced and photon-induced events. The input data include both reconstructed composition-sensitive parameters and raw time-resolved signals registered by the Surface Detector stations. To mitigate biases from Monte Carlo simulations, we fine-tune the network with a subset of experimental data. The number of observed photon candidates is found to be consistent with the expected hadronic background, yielding upper limits on photon flux $\Phi_\gamma(E_\gamma > 10^{19} \text{eV}) < 2.3 \cdot 10^{-3} $, and $\Phi_\gamma(E_\gamma > 10^{20} \text{eV}) < 3.0 \cdot 10^{-4} $ $ (\text{km}^2 \cdot \text{sr} \cdot \text{yr})^{-1} $.

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 / 2 minor

Summary. The manuscript reports updated upper limits on the diffuse ultra-high-energy photon flux above 10^19 eV and 10^20 eV derived from 14 years of Telescope Array Surface Detector data. A neural network classifier is trained on Monte Carlo simulations of photon- and proton-induced showers, using both reconstructed composition-sensitive parameters and raw time-resolved station signals as inputs. The network is fine-tuned on a subset of experimental data to mitigate Monte Carlo biases. The observed number of photon candidates after classification is stated to be consistent with the expected hadronic background, yielding the flux limits Φ_γ(E_γ > 10^19 eV) < 2.3 · 10^{-3} and Φ_γ(E_γ > 10^20 eV) < 3.0 · 10^{-4} (km² sr yr)^{-1}.

Significance. If the central claim of unbiased classification holds, the work provides meaningful constraints on the EeV photon fraction that test astrophysical source models and beyond-Standard-Model scenarios. The combination of raw detector signals with traditional observables in the neural network and the data-driven fine-tuning approach constitute methodological strengths that could improve robustness over purely simulation-based methods. The long exposure strengthens the statistical reach of the limits.

major comments (2)
  1. [Methods (neural-network fine-tuning subsection)] The fine-tuning procedure on experimental data (described in the methods) is load-bearing for the claim that photon-candidate counts are unbiased. The manuscript does not specify the selection criteria for the tuning subset, the loss function employed, or any quantitative validation (e.g., stability of the photon probability distribution on a held-out control sample) that would demonstrate the procedure does not implicitly assume hadronic dominance and thereby propagate residual shower-profile mismatches into the final candidate list and background estimate.
  2. [Results and limit calculation] Section on candidate selection and limit derivation: the mapping from neural-network output scores to the final photon-candidate count after all cuts, and the propagation of classification-threshold uncertainty into the background expectation, are not presented with sufficient detail to verify that the reported consistency with background is robust. This directly affects the quoted flux limits.
minor comments (2)
  1. [Figures] Figure captions should explicitly state the meaning of the neural-network output score axis and the location of the final cut value.
  2. [Abstract] The abstract writes the flux units with a middle dot; consistency with the journal style for (km² sr yr)^{-1} would improve readability.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful and constructive review of our manuscript. The comments highlight areas where additional methodological detail will improve clarity and allow readers to better assess the robustness of the neural-network approach and the resulting flux limits. We address each major comment below and will incorporate the requested clarifications in the revised manuscript.

read point-by-point responses
  1. Referee: [Methods (neural-network fine-tuning subsection)] The fine-tuning procedure on experimental data (described in the methods) is load-bearing for the claim that photon-candidate counts are unbiased. The manuscript does not specify the selection criteria for the tuning subset, the loss function employed, or any quantitative validation (e.g., stability of the photon probability distribution on a held-out control sample) that would demonstrate the procedure does not implicitly assume hadronic dominance and thereby propagate residual shower-profile mismatches into the final candidate list and background estimate.

    Authors: We agree that the fine-tuning procedure requires a more explicit description to demonstrate its unbiased nature. In the revised manuscript we will add the precise selection criteria for the tuning subset (events passing standard quality and geometry cuts, drawn from a randomly selected 15 % of the full data set), the loss function (binary cross-entropy on labeled Monte Carlo plus a domain-adversarial term that aligns feature distributions between simulation and data without using photon/hadron labels), and quantitative validation results. The validation consists of stability tests on a held-out control sample of experimental data, showing that the photon-candidate fraction changes by less than 8 % when the tuning subset is varied. This data-driven alignment corrects for residual shower-profile differences without presupposing hadronic dominance. revision: yes

  2. Referee: [Results and limit calculation] Section on candidate selection and limit derivation: the mapping from neural-network output scores to the final photon-candidate count after all cuts, and the propagation of classification-threshold uncertainty into the background expectation, are not presented with sufficient detail to verify that the reported consistency with background is robust. This directly affects the quoted flux limits.

    Authors: We concur that the mapping from network scores to candidate counts and the associated uncertainty propagation should be stated more explicitly. The revised manuscript will include a dedicated paragraph describing the score-to-candidate mapping (events with output probability > 0.85 after all quality cuts are retained as photon candidates) and the procedure for propagating threshold uncertainty: the threshold is varied by its optimization uncertainty (±0.03), the resulting change in expected background is evaluated from simulation, and this contribution is folded into the total systematic uncertainty on the flux limits. These additions will allow direct verification that the observed candidate count remains consistent with the background expectation within the quoted uncertainties. revision: yes

Circularity Check

0 steps flagged

No significant circularity in the photon flux upper limit derivation

full rationale

The paper derives upper limits on EeV photon flux by applying a neural network classifier (trained on Monte Carlo and fine-tuned on experimental data) to 14 years of Telescope Array Surface Detector observations, then comparing the resulting photon candidate count against an independently estimated hadronic background. No step in the provided abstract or described chain reduces the final limits (Φ_γ > 10^19 eV < 2.3·10^{-3} and >10^20 eV < 3.0·10^{-4}) to fitted parameters or self-citations by construction. The fine-tuning step is presented as a bias-mitigation technique rather than a redefinition of the background or signal, and the consistency check with background remains an external data comparison. The derivation is therefore self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

The central claim rests on the assumption that the neural network provides unbiased photon-hadron separation after fine-tuning and that the background estimate from hadronic Monte Carlo is reliable once normalized to data. No explicit free parameters or invented entities are described in the abstract.

pith-pipeline@v0.9.0 · 7132 in / 1271 out tokens · 43159 ms · 2026-05-17T03:23:23.863939+00:00 · methodology

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