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arxiv: 2510.01927 · v3 · submitted 2025-10-02 · ✦ hep-ex

Constraints on sub-GeV dark matter scattering on electrons with COSINE-100

Pith reviewed 2026-05-18 10:56 UTC · model grok-4.3

classification ✦ hep-ex
keywords sub-GeV dark matterelectron scatteringCOSINE-100NaI(Tl)upper limitsvector mediatordark matter constraints
0
0 comments X p. Extension

The pith

COSINE-100 data exclude dark matter-electron scattering cross sections above 6.4 × 10^{-33} cm² for 0.25 GeV dark matter with a light mediator.

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

The paper reports results from a dedicated search for interactions between sub-GeV dark matter particles and electrons in the sodium iodide crystals of the COSINE-100 detector. With 2.82 years of data and a total exposure of 172.9 kg-year, the analysis found no events in excess of the predicted background. This null result is used to derive 90% confidence level upper limits on the DM-electron scattering cross section under two benchmark scenarios, one with a light vector boson mediator and one with a heavy vector boson mediator. The limits are presented as the strongest constraints achieved so far with a NaI(Tl) target. The work also notes plans to push the search to lower energies with an annual modulation analysis.

Core claim

With a total exposure of 172.9 kg-year, the COSINE-100 experiment observed no excess events over the expected background in its search for sub-GeV dark matter scattering on electrons. This null result translates to 90% CL upper limits that exclude DM-electron scattering cross sections above 6.4 × 10^{-33} cm² for a 0.25 GeV DM mass assuming a light mediator, and above 3.4 × 10^{-37} cm² for a 0.4 GeV DM mass assuming a heavy mediator.

What carries the argument

Low-energy event selection and background modeling applied to NaI(Tl) scintillator data in two benchmark models of vector-boson-mediated DM-electron scattering.

Load-bearing premise

The background model accurately predicts all non-DM events in the low-energy region, with no unaccounted systematics or signal-like fluctuations that could mimic or mask a dark matter contribution.

What would settle it

A statistically significant excess of low-energy events above the predicted background rate, at a level consistent with the excluded cross sections, would invalidate the null-result limits.

Figures

Figures reproduced from arXiv: 2510.01927 by A. C. Ezeribe, B. B. Manzato, B. H. Kim, B. R. Ko, C. Ha, C. Rott, D. F. F. S. Cavalcante, D. H. Lee, D. S. Leonard, D. Y. Kim, E. J. Jeon, E. K. Lee, G. H. Yu (COSINE-100 Collaboration), H. J. Kim, H. K. Park, H. Lee, H. Prihtiadi, H. S. Lee, H. S. Park, H. W. Joo, H. Y. Lee, I. S. Hahn, I. S. Lee, J. C. Park, J. Kim, J. Lee, J. S. Park, J. Y. Cho, J. Y. Lee, K. A. Shin, K. Park, K. S. Park, K. W. Kim, L. E. Franca, L. T. Truc, L. Yang, M. H. Lee, M. Kauer, M. K. Son, N. Carlin, N. J. C. Spooner, N. T. Luan, O. Gileva, R. H. Maruyama, R. L. C. Pitta, S. Choi, S. D. Park, S. H. Kim, S. H. Lee, S. J. Cho, S. J. Hollick, S. J. Ra, S. K. Kim, S. L. Olsen, S. M. Lee, V. H. A. Machado, W. G. Kang, W. K. Kim, Y. D. Kim, Y. H. Kim, Y. J. Ko, Y. J. Lee.

Figure 1
Figure 1. Figure 1: FIG. 1. Illustration of the COSINE-100 experiment. The [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Feynman diagram that represents the DM-electron [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Computed spectra in NaI considering the non [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Expected event rate in COSINE-100 NaI(Tl) de [PITH_FULL_IMAGE:figures/full_fig_p006_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Measured data for the 2.82 years data-set used in this [PITH_FULL_IMAGE:figures/full_fig_p007_5.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. Normalized posterior distribution for [PITH_FULL_IMAGE:figures/full_fig_p007_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. Upper limits for [PITH_FULL_IMAGE:figures/full_fig_p009_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: FIG. 9. Sensitivity prospects for the COSINE-100U experiment (red) considering the light mediator model (left) and heavy [PITH_FULL_IMAGE:figures/full_fig_p009_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: FIG. 10. Comparison between different methods for perform [PITH_FULL_IMAGE:figures/full_fig_p010_10.png] view at source ↗
read the original abstract

We present results of the search for sub-GeV dark matter interaction with electrons in the NaI(Tl) crystals of the COSINE-100 experiment. The two benchmark scenarios of a heavy and a light vector boson as mediator of the interaction were studied. We found no excess events over the expected background in a data-set of 2.82 years, with a total exposure of 172.9 kg-year. The derived 90% confidence level upper limits exclude a DM-electron scattering cross section above 6.4 $\times$ 10$^{-33}$ cm$^2$ for a DM mass of 0.25 GeV, assuming a light mediator; and above 3.4 $\times$ 10$^{-37}$ cm$^2$ for a 0.4 GeV DM, assuming a heavy mediator, and represent the most stringent constraints for a NaI(Tl) target to date. We also briefly discuss a planned analysis using an annual modulation method below the current 0.7 keV threshold of COSINE-100, down to few photoelectrons yield.

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

1 major / 1 minor

Summary. The manuscript reports results from the COSINE-100 NaI(Tl) experiment searching for sub-GeV dark matter scattering on electrons. Using 172.9 kg-year of data over 2.82 years, no excess events are observed above the expected background for benchmark heavy and light vector mediator scenarios. 90% CL upper limits are set excluding DM-electron cross sections above 6.4 × 10^{-33} cm² at 0.25 GeV (light mediator) and 3.4 × 10^{-37} cm² at 0.4 GeV (heavy mediator), claimed as the most stringent for a NaI(Tl) target. Plans for a future annual modulation analysis below the current 0.7 keV threshold are briefly discussed.

Significance. If the background model holds, the result provides competitive new constraints on sub-GeV DM-electron interactions using a NaI(Tl) target, which is of interest for models with electron-philic DM. The exposure and low-energy reach are strengths, and the limits are directly derived from new data rather than circular fits. The outlined modulation search could extend sensitivity, but the current limits' robustness depends on low-energy background fidelity.

major comments (1)
  1. [Background model and statistical analysis] The central claim of no excess and the derived limits rest on the background model in the sub-keV region. The abstract asserts 'no excess events over the expected background' after 172.9 kg-year but provides no details on estimation method (e.g., sideband constraints, Monte Carlo, or floating nuisance parameters below ~0.7 keV). Small unaccounted systematics here would directly shift the quoted 90% CL limits by amounts comparable to the reported values.
minor comments (1)
  1. [Outlook] The discussion of the planned annual modulation analysis below 0.7 keV is brief; adding a short quantitative estimate of expected sensitivity improvement would strengthen the outlook section.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful review and for identifying the need for greater clarity on the background model. We address the major comment point by point below and have revised the manuscript to improve the description of our methods while preserving the original scientific content.

read point-by-point responses
  1. Referee: [Background model and statistical analysis] The central claim of no excess and the derived limits rest on the background model in the sub-keV region. The abstract asserts 'no excess events over the expected background' after 172.9 kg-year but provides no details on estimation method (e.g., sideband constraints, Monte Carlo, or floating nuisance parameters below ~0.7 keV). Small unaccounted systematics here would directly shift the quoted 90% CL limits by amounts comparable to the reported values.

    Authors: We agree that the background model in the sub-keV region is central to the result and that the abstract is necessarily brief. The full manuscript details the background estimation in Section 4: a data-driven sideband fit above 0.7 keV is used to constrain the dominant components, which are then extrapolated to lower energies with Monte Carlo simulations of known radioactive and cosmogenic backgrounds; nuisance parameters for normalization and shape uncertainties are floated in the binned likelihood fit. To address the referee's concern directly, we have added a concise summary of this procedure to the abstract and inserted a new paragraph in the analysis section that explicitly describes the constraints applied below 0.7 keV. We have also expanded the systematic uncertainty discussion to quantify how residual modeling uncertainties propagate into the 90% CL limits. These revisions make the method more transparent without changing the reported limits or conclusions. revision: yes

Circularity Check

0 steps flagged

No significant circularity in experimental limit derivation

full rationale

The paper reports new data from the COSINE-100 NaI(Tl) experiment with 172.9 kg-year exposure, constructs a background model from known sources (radioactivity, PMT noise, cosmogenic activation), observes no excess events, and derives 90% CL upper limits on DM-electron scattering cross sections using standard statistical procedures for two mediator scenarios. These limits depend on the observed counts, efficiency, and external halo model assumptions but do not reduce by construction to prior fitted parameters, self-definitions, or load-bearing self-citations. The derivation chain remains self-contained against external benchmarks and data.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

Based solely on the abstract; the central claim depends on standard domain assumptions for dark matter direct detection (halo velocity distribution, local density, mediator form factors) and accurate background subtraction. No new free parameters or invented entities are identifiable from the given text.

axioms (2)
  • domain assumption Standard galactic dark matter halo model and local density assumptions are used to convert observed rates into cross-section limits.
    Common in the field but not detailed or justified in the abstract.
  • domain assumption Background events are correctly modeled and subtracted with no significant unaccounted systematics in the sub-keV region.
    Central to the 'no excess' statement; details absent from abstract.

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