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Very Heavy and Composite Dark Matter: Theory and Experimental Searches

Joseph Bramante

Abstract

Dark matter much heavier than the weak scale remains a comparatively unexplored frontier. This review surveys theoretical and experimental developments on very heavy dark matter, including composite and dissipative formation mechanisms, multiscatter detection, and astrophysical searches.

Very Heavy and Composite Dark Matter: Theory and Experimental Searches

Abstract

Dark matter much heavier than the weak scale remains a comparatively unexplored frontier. This review surveys theoretical and experimental developments on very heavy dark matter, including composite and dissipative formation mechanisms, multiscatter detection, and astrophysical searches.
Paper Structure (25 sections, 22 equations, 6 figures)

This paper contains 25 sections, 22 equations, 6 figures.

Figures (6)

  • Figure 1: Composite formation pathways for dark matter. Top: hierarchical radiative dark nucleosynthesis, where two-body bound states form through mediator emission and merge into larger composites, radiating a scalar $\phi$ at each fusion step. Middle: dissipative formation and fragmentation of dark compact objects, adapted from Fig. 1 of Bramante:2024pyc, which shows a sequence of dark halo virialization, radiative cooling, fragmentation, dilution, and low-redshift compact remnant formation. Bottom: composite formation in a first-order phase transition, where shrinking bubbles of the high temperature phase trap and compress dark constituents.
  • Figure 2: Multiscatter phenomenology of very heavy dark matter. Left: schematic of multiple nuclear recoils aligned along a single linear trajectory for $m_X\!\gg\!m_N$, producing a correlated light or charge track Bramante:2018tos. Right: exclusion region from the DEAP-3600 multiscatter search DEAPCollaboration:2021raj, constraining dark matter masses up to $10^{19}\,\mathrm{GeV}$. The enclosed region is bounded below by the minimum cross-section required to produce a detectable multiscatter track using the pulse-timing discrimination analysis at DEAP-3600, above by energy attenuation in the Earth's overburden, and on the right by the local dark matter flux. Variations in the terminus of the right boundary depend on DEAP-3600 sensitivity to different energy thresholds/high-velocity phase space of dark matter.
  • Figure 3: Schematic regimes of composite dark matter scattering in detectors. Four conceptual panels are shown from left to right: (1.) Whole-composite boundary acceleration: an incoming dark composite interacts coherently with a nucleus, transferring momentum to the entire bound state and producing nuclear recoil radiation; (2.) Soft boundary recoils and Migdal emission: partial or glancing interactions excite electrons and emit soft bremsstrahlung photons, leading to correlated electronic signals along the track; (3.) Reflection or saturation regime: for large effective mediator field or large $|\langle\varphi\rangle|$, the scattering becomes surface-dominated and the momentum transfer saturates near the geometric limit; (4.) Loosely bound composite regime: the probe resolves individual constituents within an extended dark bound state, producing incoherent constituent-level scattering as described in Sec. \ref{['subsec:looselybound']}. Adapted from Fig. 1 of Acevedo:2021kly, with the final panel illustrating the loosely bound composite regime explored in Acevedo:2024lyr.
  • Figure 4: Some multiscatter and high-mass dark matter limits from terrestrial detectors. Left: Chicago EJ-301 coincidence search Cappiello:2020lbk; Right: LZ multiscatter search LZ:2024psa. The relatively flat lower bound of the EJ-301 search is determined by a threshold for total nuclear recoil deposition in a liquid scintillator detector, while the LZ SR1 multiscatter search has a more characteristic $1/ m_X$ scaling of a single-recoil sensitive detector.
  • Figure 5: Etched plastic and ancient mica constraints on very heavy or composite dark matter. Excavated ancient mica limits for the per-nucleon (left) and nucleon-independent (right) parameterizations are shown in blue and red Acevedo:2021tbl alongside etched-plastic limits in gray (labeled Skylab and Ohya) from Bhoonah:2020fys. Both studies incorporated overburden attenuation and detector thresholds - the features apparent in the red mica bounds result from a detailed Monte Carlo of dark matter attenuation through the Earth's crust Acevedo:2021tbl, whereas the plastic etch bounds have more uniform overburden material Bhoonah:2020fys. A broader overview of mineral-based searches is given in Baum:2023cct.
  • ...and 1 more figures