- Open Access
Probing Benchmark Models of Hidden-Sector Dark Matter with DAMIC-M
Phys. Rev. Lett. 135, 071002 – Published 13 August, 2025
DOI: https://doi.org/10.1103/2tcc-bqck
Abstract
We report on a search for sub-GeV dark matter (DM) particles interacting with electrons using the DAMIC-M prototype detector at the Modane Underground Laboratory. The data feature a significantly lower detector single rate (factor 50) compared to our previous search, while also accumulating a 10 times larger exposure of . DM interactions in the skipper charge-coupled devices (CCDs) are searched for as groups of two or three adjacent pixels with a total charge between 2 and . We find 144 candidates of and 1 candidate of , where 141.5 and 0.071, respectively, are expected from background. With no evidence of a DM signal, we place stringent constraints on DM particles with masses between 1 and interacting with electrons through an ultralight or heavy mediator. For large ranges of DM masses below , we exclude theoretically motivated benchmark scenarios where hidden-sector particles are produced as a major component of DM in the Universe through the freeze-in or freeze-out mechanisms.
Physics Subject Headings (PhySH)
Corrections
19 December, 2025
Correction: A grant number was missing from the third sentence of the Acknowledgments and has been inserted.
See Also
Daily modulation constraints on light dark matter with DAMIC-M
Article Text
References (89)
- G. Bertone, D. Hooper, and J. Silk, Phys. Rep. 405, 279 (2005).
- A. Drukier and L. Stodolsky, Phys. Rev. D 30, 2295 (1984).
- M. W. Goodman and E. Witten, Phys. Rev. D 31, 3059 (1985).
- A. K. Drukier, K. Freese, and D. N. Spergel, Phys. Rev. D 33, 3495 (1986).
- J. Billard et al., Rep. Prog. Phys. 85, 056201 (2022).
- C. Boehm, P. Fayet, and J. Silk, Phys. Rev. D 69, 101302(R) (2004).
- D. Hooper and K. M. Zurek, Phys. Rev. D 77, 087302 (2008).
- M. Pospelov, A. Ritz, and M. B. Voloshin, Phys. Lett. B 662, 53 (2008).
- X. Chu, T. Hambye, and M. H. G. Tytgat, J. Cosmol. Astropart. Phys. 05 (2012) 034.
- S. Knapen, T. Lin, and K. M. Zurek, Phys. Rev. D 96, 115021 (2017).
- R. Essig, J. Mardon, and T. Volansky, Phys. Rev. D 85, 076007 (2012).
- R. Essig, M. Fernandez-Serra, J. Mardon, A. Soto, T. Volansky, and T.-T. Yu, J. High Energy Phys. 05 (2016) 046.
- B. Holdom, Phys. Lett. 166B, 196 (1986).
- L. B. Okun, Sov. Phys. JETP 56, 502 (1982), https://ui.adsabs.harvard.edu/abs/1982ZhETF..83..892O/abstract.
- C. E. Dreyer, R. Essig, M. Fernandez-Serra, A. Singal, and C. Zhen, Phys. Rev. D 109, 115008 (2024).
- S. K. Lee, M. Lisanti, S. Mishra-Sharma, and B. R. Safdi, Phys. Rev. D 92, 083517 (2015).
- S. M. Griffin, K. Inzani, T. Trickle, Z. Zhang, and K. M. Zurek, Phys. Rev. D 104, 095015 (2021).
- T. Emken, R. Essig, C. Kouvaris, and M. Sholapurkar, J. Cosmol. Astropart. Phys. 09 (2019) 070.
- L. J. Hall, K. Jedamzik, J. March-Russell, and S. M. West, J. High Energy Phys. 03 (2010) 080.
- E. Izaguirre, G. Krnjaic, P. Schuster, and N. Toro, Phys. Rev. Lett. 115, 251301 (2015).
- M. Battaglieri et al., arXiv:1707.04591.
- C. Dvorkin, T. Lin, and K. Schutz, Phys. Rev. D 99, 115009 (2019).
- C. Dvorkin, T. Lin, and K. Schutz, Phys. Rev. D 105, 119901(E) (2022).
- P. N. Bhattiprolu, R. McGehee, and A. Pierce, Phys. Rev. D 110, L031702 (2024).
- I. Arnquist et al. (DAMIC-M Collaboration), Phys. Rev. Lett. 130, 171003 (2023).
- I. Arnquist et al. (DAMIC-M Collaboration), Phys. Rev. Lett. 132, 101006 (2024).
- P. Agnes et al. (DarkSide Collaboration), Phys. Rev. Lett. 130, 101002 (2023).
- S. Li et al. (PandaX Collaboration), Phys. Rev. Lett. 130, 261001 (2023).
- P. Adari et al. (SENSEI Collaboration), Phys. Rev. Lett. 134, 011804 (2025).
- M. F. Albakry et al., Phys. Rev. D 111, 012006 (2025).
- E. Aprile et al., Phys. Rev. Lett. 134, 161004 (2025).
- E. Aprile et al. (XENON Collaboration), Phys. Rev. Lett. 123, 251801 (2019).
- A. Aguilar-Arevalo et al. (DAMIC Collaboration), Phys. Rev. Lett. 123, 181802 (2019).
- Q. Arnaud et al. (EDELWEISS Collaboration), Phys. Rev. Lett. 125, 141301 (2020).
- R. Agnese et al. (SuperCDMS Collaboration), Phys. Rev. Lett. 121, 051301 (2018); 122, 069901(E) (2019).
- Z. Y. Zhang et al. (CDEX Collaboration), Phys. Rev. Lett. 129, 221301 (2022).
- P. Privitera, Proc. Sci. TAUP2023 (2024) 066.
- I. Arnquist et al. (DAMIC-M Collaboration), J. Instrum. 19, T11010 (2024).
Laboratoire Souterrain de Modane.
- S. E. Holland, Exp. Astron. 14, 83 (2002).
- S. E. Holland, D. E. Groom, N. P. Palaio, R. J. Stover, and M. Wei, IEEE Trans. Electron Devices 50, 225 (2003).
- S. E. Holland, W. F. Kolbe, and C. J. Bebek, IEEE Trans. Electron Devices 56, 2612 (2009).
- A. Alessandrello, C. Cattadori, G. Fiorentini, E. Fiorini, G. Gervasio, G. Heusser, G. Mezzorani, E. Pernicka, P. Quarati, D. Salvi, P. Sverzellati, and L. Zanotti, Nucl. Instrum. Methods Phys. Res., Sect. B 61, 106 (1991).
- A. Aguilar-Arevalo et al. (DAMIC Collaboration), Phys. Rev. D 94, 082006 (2016).
- J. Janesick, T. Elliott, A. Dingiziam, R. Bredthauer, C. Chandler, J. Westphal, and J. Gunn, Proc. SPIE Int. Soc. Opt. Eng. 1242, 223 (1990).
- C. E. Chandler, R. A. Bredthauer, J. R. Janesick, J. A. Westphal, and J. E. Gunn, Proc. SPIE Int. Soc. Opt. Eng. 1242, 238 (1990).
- J. Tiffenberg, M. Sofo-Haro, A. Drlica-Wagner, R. Essig, Y. Guardincerri, S. Holland, T. Volansky, and T.-T. Yu, Phys. Rev. Lett. 119, 131802 (2017).
The readout noise of skipper CCDs is sensitive to electrical grounding, which was not fully optimized at that time. After an intervention following the completion of the data taking period, we achieved with the shielding fully closed.
We read out more columns than the 6144 physical ones of the CCD. These additional pixels, which have much lower exposure, provide useful information on data quality and dark current in the serial register.
- J. R. Janesick, Scientific Charge-Coupled Devices (SPIE Optical Engineering Press, Bellingham, WA, 2001).
We define the charge q of a pixel to be when q .
- S. Agostinelli et al., Nucl. Instrum. Methods Phys. Res., Sect. A 506, 250 (2003).
- K. Ramanathan and N. Kurinsky, Phys. Rev. D 102, 063026 (2020).
- A. Aguilar-Arevalo et al. (DAMIC Collaboration), Phys. Rev. D 105, 062003 (2022).
, with parameters , , , and .
- A. Aguilar-Arevalo et al. (DAMIC, DAMIC-M, and SENSEI Collaborations), Phys. Rev. D 109, 062007 (2024).
- G. Cowan, K. Cranmer, E. Gross, and O. Vitells, Eur. Phys. J. C 71, 1554 (2011); 73, 2501(E) (2013).
- D. Baxter et al., Eur. Phys. J. C 81, 907 (2021).
For better legibility of the figures we include only the most recent results. Other exclusion limits can be found in Refs. [33–36,60] Other solar-reflected DM limits can be found in Refs. [31,61–63].
- R. Essig, T. Volansky, and T.-T. Yu, Phys. Rev. D 96, 043017 (2017).
- H. An, H. Nie, M. Pospelov, J. Pradler, and A. Ritz, Phys. Rev. D 104, 103026 (2021).
- T. Emken, Phys. Rev. D 105, 063020 (2022).
- Z. Y. Zhang et al. (CDEX Collaboration), Phys. Rev. Lett. 132, 171001 (2024).
- T. Emken, R. Essig, and H. Xu, J. Cosmol. Astropart. Phys. 07 (2024) 023.
We calculate the effects of Earth-shielding using the verne code [66], assuming that the mediator is a dark photon and that scattering off nuclei dominate the shielding effect [18].
- B. J. Kavanagh, Phys. Rev. D 97, 123013 (2018).
For CCD 1-C, after Step 6 because of columns being masked; when this is taken into account, the fraction of surviving pixels is still around 95%.
- S. Knapen, J. Kozaczuk, and T. Lin, Phys. Rev. D 105, 015014 (2022).
- T. Trickle, Phys. Rev. D 107, 035035 (2023).
- The DAMIC-M 90% C.L. exclusion limits obtained for several DM candidates and different calculations of the DM- interaction rate can be found at https://github.com/DAMIC-M/LBC_2025_HSBenchmark_Limits.
- M. Fabbrichesi, E. Gabrielli, and G. Lanfranchi, The Physics of the Dark Photon: A Primer (Springer International Publishing, New York, 2021).
- J. D. Vergados and H. Ejiri, Phys. Lett. B 606, 313 (2005).
- C. C. Moustakidis, J. D. Vergados, and H. Ejiri, Nucl. Phys. B727, 406 (2005).
- R. Bernabei et al., Int. J. Mod. Phys. A 22, 3155 (2007).
- M. Ibe, W. Nakano, Y. Shoji, and K. Suzuki, J. High Energy Phys. 03 (2018) 194.
- P. Agnes et al. (DarkSide Collaboration), Phys. Rev. Lett. 130, 101001 (2023).
- D. Huang et al. (PandaX Collaboration), Phys. Rev. Lett. 131, 191002 (2023).
- M. F. Albakry et al. (SuperCDMS Collaboration), Phys. Rev. D 107, 112013 (2023).
- E. Aprile et al. (XENON Collaboration), Phys. Rev. Lett. 123, 241803 (2019).
- I. M. Bloch, R. Essig, K. Tobioka, T. Volansky, and T.-T. Yu, J. High Energy Phys. 06 (2017) 087.
- A. H. Abdelhameed et al. (CRESST Collaboration), Phys. Rev. D 100, 102002 (2019).
- G. Angloher et al. (CRESST Collaboration), Phys. Rev. D 110, 083038 (2024).
- I. Alkhatib et al. (SuperCDMS Collaboration), Phys. Rev. Lett. 127, 061801 (2021).
- S. Knapen, J. Kozaczuk, and T. Lin, Phys. Rev. D 105, 015014 (2022).
- A. Aguilar-Arevalo et al. (DAMIC Collaboration), Phys. Rev. Lett. 118, 141803 (2017).
- D. F. Edwards, in Handbook of Optical Constants of Solids, edited by E. D. Palik (Academic Press, Burlington, 1997), pp. 547–569.
- K. Rajkanan, R. Singh, and J. Shewchun, Solid-State Electron. 22, 793 (1979).
- K. Berghaus, A. Esposito, R. Essig, and M. Sholapurkar, J. High Energy Phys. 01 (2023) 023.
- J. Enkovaara et al., J. Phys. Condens. Matter 22, 253202 (2010).