pith. sign in

arxiv: 2605.15739 · v2 · pith:SOY7A3DBnew · submitted 2026-05-15 · ⚛️ physics.ins-det · hep-ex

R&D of cosmic ray detection module with liquid scintillator and wavelength shift fiber

Pith reviewed 2026-05-21 08:56 UTC · model grok-4.3

classification ⚛️ physics.ins-det hep-ex
keywords cosmic ray detectionliquid scintillatorwavelength-shifting fibermuon taggingbackground rejectionneutrino physicsrare event searches
0
0 comments X

The pith

Liquid scintillator and wavelength-shifting fiber module achieves good photoelectron response in muon prototype tests.

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

The paper develops a cosmic ray detection module using liquid scintillator and wavelength-shifting fibers to tag muons and suppress backgrounds in neutrino physics and rare-event searches. The design focuses on keeping costs manageable while delivering usable performance for large detector arrays. Measurements on a small prototype exposed to cosmic muons show effective photoelectron collection from the scintillator. This outcome indicates the module can serve as a practical tool for identifying cosmic rays in underground experiments. If the performance holds at larger scales, the approach could support background control in future observatories.

Core claim

The central claim is that a detection module consisting of liquid scintillator read out via wavelength-shifting fibers produces good photoelectron response when tested with muons, establishing its suitability for cost-effective cosmic ray identification and rejection in large-scale setups for particle physics and astrophysics applications.

What carries the argument

The liquid scintillator and wavelength-shifting fiber module, which converts muon energy deposits into optical signals collected for detection.

If this is right

  • Enables reliable muon tagging to reduce cosmic-ray backgrounds in neutrino detectors.
  • Provides a lower-cost alternative for building extensive cosmic ray veto systems.
  • Supports underground rare-event experiments by improving background rejection rates.
  • Supplies design data for optimizing fiber placement and scintillator volume in future modules.

Where Pith is reading between the lines

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

  • The module could be combined with existing water-Cherenkov or tracking detectors to create hybrid veto layers.
  • Production scaling might allow deployment in experiments requiring hundreds of square meters of coverage.
  • Light-yield modeling from the prototype could guide adjustments to fiber density for different muon energies.

Load-bearing premise

The good photoelectron response seen in the small prototype will continue in larger arrays while preserving reasonable costs and without major drops in efficiency or uniformity.

What would settle it

A scaled-up module showing markedly lower light yield, poor uniformity across its area, or unexpectedly high costs would falsify the claim that the design is viable for large arrays.

read the original abstract

For neutrino physics and rare event searches, background related to cosmic muons poses a notable challenge, and must be identified and rejected. It is also a challenge to control the cost with good performance for a large array of cosmic ray detection. We proposed a cosmic ray detection module with liquid scintillator and wavelength-shifting fibers for its reasonable cost and performances. The results from the measurements of a prototype with Muon indicate that the detector's photoelectron response is good. % comparing to the expectation. The outcomes of this study hold significant potential for applications in cosmic ray observation experiments and underground rare-event detection, providing a viable option for future large-scale observatories. This work highlights the feasibility of liquid scintillator-based detectors in addressing current and emerging challenges in particle physics and astrophysics.

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 paper proposes a cosmic ray detection module using liquid scintillator and wavelength-shifting fibers as a cost-effective option for large veto arrays in neutrino physics and rare-event searches. A small prototype was constructed and tested with muons; the authors report that the measured photoelectron response is good and conclude that the approach is feasible for future large-scale observatories.

Significance. If the prototype performance holds at scale, the design could provide a practical, lower-cost alternative for cosmic-ray veto systems in underground experiments. The work is a standard experimental R&D contribution that directly addresses a known engineering challenge in the field, though its impact depends on quantitative validation and scaling studies that are not yet presented.

major comments (2)
  1. [Abstract / prototype measurements] Abstract and prototype-results section: the statement that 'the detector's photoelectron response is good' is presented without numerical values for photoelectron yield, light-collection efficiency, comparison to Monte Carlo expectations, error bars, or muon-selection criteria. This absence prevents quantitative assessment of the central performance claim.
  2. [Discussion / conclusions] Discussion and conclusions: no data, simulation, or scaling argument is supplied for light-collection uniformity, fiber attenuation, or per-unit-area efficiency when module area or fiber count is increased by the factors required for large underground arrays. This extrapolation is load-bearing for the claim of applicability to 'large-scale observatories' yet remains untested.
minor comments (2)
  1. [Abstract] The abstract contains the stray fragment '% comparing to the expectation.' which should be removed or completed.
  2. [Figures / experimental setup] Figure captions and text should explicitly state the active area of the prototype, number of fibers, and scintillator volume so that readers can judge the scale of the reported measurement.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive comments, which help improve the clarity and rigor of our presentation. We address each major comment below and have revised the manuscript to incorporate additional quantitative details and discussion where feasible.

read point-by-point responses
  1. Referee: [Abstract / prototype measurements] Abstract and prototype-results section: the statement that 'the detector's photoelectron response is good' is presented without numerical values for photoelectron yield, light-collection efficiency, comparison to Monte Carlo expectations, error bars, or muon-selection criteria. This absence prevents quantitative assessment of the central performance claim.

    Authors: We agree that the original wording was insufficiently quantitative. The revised manuscript now includes the measured photoelectron yield per muon (with statistical and systematic uncertainties), the estimated light-collection efficiency, the specific muon-selection criteria applied to the data, and a direct comparison of the observed response to Monte Carlo expectations. These values are drawn from the prototype dataset described in the results section. revision: yes

  2. Referee: [Discussion / conclusions] Discussion and conclusions: no data, simulation, or scaling argument is supplied for light-collection uniformity, fiber attenuation, or per-unit-area efficiency when module area or fiber count is increased by the factors required for large underground arrays. This extrapolation is load-bearing for the claim of applicability to 'large-scale observatories' yet remains untested.

    Authors: We acknowledge that the original manuscript did not provide explicit scaling arguments. In the revised version we have added a dedicated paragraph in the discussion that reports the measured fiber attenuation length and uniformity across the prototype, together with a simple scaling estimate based on these data. We also note the limitations of the current prototype and outline the additional measurements required before claiming readiness for large arrays; the applicability statement has been tempered accordingly. revision: partial

Circularity Check

0 steps flagged

No significant circularity in experimental R&D report

full rationale

This paper is a straightforward experimental report on the construction and muon testing of a small liquid-scintillator + WLS-fiber prototype. The central claim rests on direct measurements of photoelectron yield rather than any derivation, model, or fitted parameter. No equations, ansatzes, self-citations used as load-bearing premises, or predictions that reduce to the input data by construction appear in the provided text. The work is self-contained against its own empirical benchmarks and does not invoke uniqueness theorems or prior author results to justify its conclusions.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

No free parameters, axioms, or invented entities are identifiable from the abstract alone; the work relies on standard assumptions about scintillator light yield and muon interactions that are established in the broader field.

pith-pipeline@v0.9.0 · 5703 in / 1067 out tokens · 56888 ms · 2026-05-21T08:56:20.231681+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

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

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.

Reference graph

Works this paper leans on

22 extracted references · 22 canonical work pages

  1. [1]

    Collaboration,Juno physics and detector,Progress in Particle and Nuclear Physics123(2022) 103927

    J. Collaboration,Juno physics and detector,Progress in Particle and Nuclear Physics123(2022) 103927

  2. [2]

    Collaboration, A

    J. Collaboration, A. Abusleme, T. Adam, S. Ahmad, S. Aiello, M. Akram et al.,Tao conceptual design report: A precision measurement of the reactor antineutrino spectrum with sub-percent energy resolution, 2020.https://arxiv.org/abs/2005.08745

  3. [3]

    Luo et al.,Design optimization of plastic scintillators with wavelength-shifting fibers and silicon photomultiplier readouts in the top veto tracker of the JUNO-TAO experiment,Nucl

    G. Luo et al.,Design optimization of plastic scintillators with wavelength-shifting fibers and silicon photomultiplier readouts in the top veto tracker of the JUNO-TAO experiment,Nucl. Sci. Tech.34 (2023) 99 [2302.12669]

  4. [4]

    Luo, X.-H

    G. Luo, X.-H. Yin, F.-P. An, Z.-M. Wang, Y.K. Hor, P.-Z. Lu et al.,Performance of plastic scintillator modulesfortopvetotrackeratTaishanAntineutrinoObservatory,NuclearScienceandTechniques36 (2025) 91

  5. [5]

    C. Zhen, C. Ming-jun, C. Song-zhan, H. Hong-bo, L. Cheng, L. Ye et al.,Introduction to large high altitude air shower observatory (lhaaso),Chinese Astronomy and Astrophysics43(2019) 457

  6. [6]

    Zhang, J

    Y. Zhang, J. Xu, H. Lu, P. Zhang, C. Zhang and C. Yang,Discriminating cosmic muons and radioactivity using a liquid scintillation fiber detector,Journal of Instrumentation12(2017) P03015

  7. [7]

    Zhang, J

    Y. Zhang, J. Huang, D. Chen, L. Zhai, Y. Meng, K. Hu et al.,Design and optimization of a liquid scintillator detector for new eas hybrid experiment,Journal of Instrumentation20(2025) P06017

  8. [8]

    State-key-laboratory-of-particle-detection-and-electronics

    S.-K.-L. of-Particle-Detection-and Electronics, “State-key-laboratory-of-particle-detection-and-electronics.” http://english.ihep.cas.cn/se/kl/sk/

  9. [9]

    Y.-P. Wang, C. Hou, X.-D. Sheng, S.-H. Feng, H.-K. Lv, J. Liu et al.,Testing and analysis of the plasticscintillatorunitsforLHAASO-ED,RadiationDetectionTechnologyandMethods5(2021)513

  10. [10]

    Y. Ding, Z. Zhang, J. Liu, Z. Wang, P. Zhou and Y. Zhao,A new gadolinium-loaded liquid scintillator for reactor neutrino detection,Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment584(2008) 238

  11. [11]

    M. Yeh, A. Garnov and R.L. Hahn,Gadolinium-loaded liquid scintillator for high-precision measurements of antineutrino oscillations and the mixing angle,𝜃13,Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment578(2007) 329

  12. [12]

    LUXIUM, “Bcf-92.”https://luxiumsolutions.com/

  13. [13]

    Dupont, “Tyvek.”https://www.dupont.com/content/dam/dupont/amer/us/en/ microsites/tyvek-design/images/documents/CN-China-Tyvek(r) -Graphics-Printing&Technical-Guide-2020.pdf

  14. [14]

    [15]LHAASOcollaboration,Batch Measurement of Attenuation Length of Wavelength-shifting Fibers for LHAASO Electromagnetic Detectors,PoSICRC2019(2020) 490

    “Nim.”https://www.nim.ac.cn/. [15]LHAASOcollaboration,Batch Measurement of Attenuation Length of Wavelength-shifting Fibers for LHAASO Electromagnetic Detectors,PoSICRC2019(2020) 490. – 14 –

  15. [15]

    C. Cao, J. Xu, M. He, A. Abusleme, M. Bongrand, C. Bordereau et al.,Mass production and characterization of 3-inch pmts for the juno experiment,Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment1005(2021) 165347

  16. [16]

    Wang and O

    Z. Wang and O. behalf of the JUNO Collaboration,Juno pmt system and prototyping,Journal of Physics: Conference Series888(2017) 012052

  17. [17]

    N. Li, Y. kun Heng, M. He, J. lei Xu, X. tong Zhang, C. ya Cao et al.,Characterization of 3-inch photomultiplier tubes for the juno central detector,Radiation Detection Technology and Methods3 (2019) 6

  18. [18]

    D. Wu, J. Xu, M. He, Z. Wang and Z. Chu,Study of the front-end signal for the 3-inch PMTs instrumentation in JUNO,Radiation Detection Technology and Methods6(2022) 349

  19. [19]

    CAEN, “Dt5743.”https://www.caen.it/products/dt5743/

  20. [20]

    “Geant4.”https://geant4.web.cern.ch/

  21. [21]

    Abusleme, T

    A. Abusleme, T. Adam et al.,Optimization of the juno liquid scintillator composition using a daya bay antineutrino detector,Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment988(2021) 164823

  22. [22]

    Cao and et

    C. Cao and et. al.,Mass production and characterization of 3-inch pmts for the juno experiment, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment1005(2021) 165347. – 15 –