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PreprintCC BY 4.0arXiv

A Freeze-In Interpretation of the LZ High-Energy Nuclear Recoil Event

Abstract

The recent LUX-ZEPLIN (LZ) experiment analysis reported a high energy nuclear recoil candidate at ER ≃ 248 keV, motivating interpretations in terms of inelastic dark matter. We study this event in a pseudo-Dirac fermion model with a vector boson mediator Z', assuming a low-reheating temperature and dark matter production through freeze-in at stronger coupling. In contrast to the thermal freeze-out case, the reheating temperature provides an additional parameter controlling the relic abundance and breaks the one-to-one relation between the dark matter mass and direct-detection cross section. As a result, the LZ candidate can be reproduced over a continuous region of parameter space, including mass splitting below the thermal benchmark.

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BibTeX
@misc{caboalmeida2026freezein,
  title = {{A Freeze-In Interpretation of the LZ High-Energy Nuclear Recoil Event}},
  author = {D. Cabo-Almeida and F. Costa and D. Feiteira and V. Oliveira},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2609.13130},
  eprint = {2609.13130},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.13130},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - A Freeze-In Interpretation of the LZ High-Energy Nuclear Recoil Event
AU  - D. Cabo-Almeida
AU  - F. Costa
AU  - D. Feiteira
AU  - V. Oliveira
PY  - 2026
DA  - 2026/10/02
PB  - arXiv
DO  - 10.48550/arxiv.2609.13130
UR  - https://arxiv.org/abs/2609.13130
AB  - The recent LUX-ZEPLIN (LZ) experiment analysis reported a high energy nuclear recoil candidate at E_R ≃ 248 keV, motivating interpretations in terms of inelastic dark matter. We study this event in a pseudo-Dirac fermion model with a vector boson mediator Z', assuming a low-reheating temperature and dark matter production through freeze-in at stronger coupling. In contrast to the thermal freeze-out case, the reheating temperature provides an additional parameter controlling the relic abundance and breaks the one-to-one relation between the dark matter mass and direct-detection cross section. As a result, the LZ candidate can be reproduced over a continuous region of parameter space, including mass splitting below the thermal benchmark.
ER  -