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Direct detection of dark matter in universal bound states
High Energy Physics - Phenomenology · Submitted 25 Nov 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim If these features are observed in experiments, it will give a smoking-gun signature for the internal structure of dark matter.
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The abstract, sentence by sentence
We study the signatures for internal structure of dark matter in direct detection experiments in the context of asymmetric self-interacting dark matter. The self-interaction cross section of two dark matter particles at low energies is assumed to come close to saturating the S-wave unitarity bound, which requires the presence of a resonance near their scattering threshold. The universality of S-wave near-threshold resonances then implies that the low-energy scattering properties of a two-body bound state of dark matter particles are completely determined by its binding energy, irrespective of the underlying microphysics. The form factor for elastic scattering of the bound state from a nucleus and the possibility of breakup of the bound state produce new signatures in the nuclear recoil energy spectrum. If these features are observed in experiments, it will give a smoking-gun signature for the internal structure of dark matter.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study the signatures for internal structure of dark matter in direct detection experiments in the context of asymmetric self-interacting dark matter. | contribution 0.99 | 0.78 | 0.06 | asserted 0.71 |
| s1 | The self-interaction cross section of two dark matter particles at low energies is assumed to come close to saturating the S-wave unitarity bound, which requires the presence of a resonance near their scattering threshold. | background 0.53 | 0.10 | 0.04 | hedged possibility 0.56 |
| s2 | The universality of S-wave near-threshold resonances then implies that the low-energy scattering properties of a two-body bound state of dark matter particles are completely determined by its binding energy, irrespective of the underlying microphysics. | background 0.45 | 0.15 | 0.29 | asserted 1.00 |
| s3 | The form factor for elastic scattering of the bound state from a nucleus and the possibility of breakup of the bound state produce new signatures in the nuclear recoil energy spectrum. | result 0.61 | 0.39 | 0.14 | asserted 0.75 |
| s4 | If these features are observed in experiments, it will give a smoking-gun signature for the internal structure of dark matter. | interpretation 1.00 | 0.07 | 0.63 | asserted 0.51 |
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The paper
Original abstract
We study the signatures for internal structure of dark matter in direct detection experiments in the context of asymmetric self-interacting dark matter. The self-interaction cross section of two dark matter particles at low energies is assumed to come close to saturating the S-wave unitarity bound, which requires the presence of a resonance near their scattering threshold. The universality of S-wave near-threshold resonances then implies that the low-energy scattering properties of a two-body bound state of dark matter particles are completely determined by its binding energy, irrespective of the underlying microphysics. The form factor for elastic scattering of the bound state from a nucleus and the possibility of breakup of the bound state produce new signatures in the nuclear recoil energy spectrum. If these features are observed in experiments, it will give a smoking-gun signature for the internal structure of dark matter.
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References
How the literature uses it
42 arXiv papers cite this in 63 sentences
Papers citing it · 40 sentences without a confident label
Compares with it 1 paper
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We then arrive at the following analytical expression for the double differential: [equation] where [equation] [equation] and [equation] Numerically integrating the expression in Eqn. [ref] over the solid angle reproduces the relevant expression in Ref. [ref] .
Directional detection of dark matter in universal bound states · Break up scattering of darkonium · 0.92
Cites it as background 17 papers
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[ref] , the issue has been investigated more systematically in a series of recent studies [ref] .
Dark Matter's secret liaisons: phenomenology of a dark U(1) sector with bound states · Introduction · 0.86
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There have been several previous applications of zero-range effective field theories to dark matter with resonant S-wave self-interactions [ref] .
Zero-Range Effective Field Theory for Resonant Wino Dark Matter I. Framework · Introduction · 0.91
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Ref. [ref] are the recent papers which had built or calculated the dark matter models in which bound state can be formed.
Dark Matter Bound State Formation in Fermionic $Z_2$ DM model with Light Dark Photon and Dark Higgs Boson · Introduction · 0.87
What it cites · 32 sentences without a confident label
Builds on 2 papers
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Given the recent excitement about self-interacting dark matter, one can try to apply the new ideas mentioned in [ref] to other respects of dark matter physics.
Universality in Few-body Systems with Large Scattering Length · Introduction · 0.84
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Given the recent excitement about self-interacting dark matter, one can try to apply the new ideas mentioned in [ref] to other respects of dark matter physics.
Universal Two-body Physics in Dark Matter near an S-wave Resonance · Introduction · 0.84
Cites as background 20 papers
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Dark matter direct detection probes the elastic scattering of dark matter particles from a nucleus at relatively low energies [ref] .
Annual Modulation of Dark Matter: A Review · Introduction · 0.99
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Dark matter direct detection probes the elastic scattering of dark matter particles from a nucleus at relatively low energies [ref] .
Generalized Analysis of Weakly-Interacting Massive Particle Searches · Introduction · 0.99
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Dark matter direct detection probes the elastic scattering of dark matter particles from a nucleus at relatively low energies [ref] .
WIMP physics with ensembles of direct-detection experiments · Introduction · 0.99
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