Endothermic Z'-Portal Dark Matter: LZ-LHC Complementarity
Abstract
Motivated by the 2.6σ high-energy recoil event recently reported by the LUX-ZEPLIN (LZ) Collaboration, we consider an endothermic Z′-portal Majorana dark matter framework and discuss the complementarity between the LZ event and LHC searches for a Z′ resonance. As a concrete realization, we consider a gauged U(1) B−L extension of the Standard Model. The phenomenology of the framework is essentially controlled by two free parameters: the U(1) B−L gauge coupling gBL and the Z′ boson mass mZ′. For a fixed mZ′, the observed dark matter abundance requires the dark matter mass to be near the Z′ resonance, mDM ∼ mZ′/2, and sets a lower bound on gBL. Complementarily, LHC searches for a Z′ resonance set an upper bound on gBL. The parameter space allowed by the dark matter abundance and LHC constraints can account for the recent LZ event. The synergy between future Z′ resonance searches at the High-Luminosity LHC and the LZ experiment may provide a test of this framework.
Related
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- Cosmological Constrained Axion-Portal Inelastic Dark Matter for the LZ Event
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BibTeX
@misc{okada2026endothermic,
title = {{Endothermic Z'-Portal Dark Matter: LZ-LHC Complementarity}},
author = {Nobuchika Okada and Digesh Raut},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.21011},
eprint = {2609.21011},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.21011},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Endothermic Z'-Portal Dark Matter: LZ-LHC Complementarity
AU - Nobuchika Okada
AU - Digesh Raut
PY - 2026
DA - 2026/09/24
PB - arXiv
DO - 10.48550/arxiv.2609.21011
UR - https://arxiv.org/abs/2609.21011
AB - Motivated by the 2.6σ high-energy recoil event recently reported by the LUX-ZEPLIN (LZ) Collaboration, we consider an endothermic Z^′-portal Majorana dark matter framework and discuss the complementarity between the LZ event and LHC searches for a Z^′ resonance. As a concrete realization, we consider a gauged U(1) B−L extension of the Standard Model. The phenomenology of the framework is essentially controlled by two free parameters: the U(1) B−L gauge coupling g_BL and the Z^′ boson mass m_Z^′. For a fixed m_Z^′, the observed dark matter abundance requires the dark matter mass to be near the Z^′ resonance, m_DM ∼ m_Z^′/2, and sets a lower bound on g_BL. Complementarily, LHC searches for a Z^′ resonance set an upper bound on g_BL. The parameter space allowed by the dark matter abundance and LHC constraints can account for the recent LZ event. The synergy between future Z^′ resonance searches at the High-Luminosity LHC and the LZ experiment may provide a test of this framework.
ER -