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Universal Two-body Physics in Dark Matter near an S-wave Resonance
High Energy Physics - Phenomenology · Submitted 19 Mar 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We point out that if the resonance is in the S-wave channel, the mechanisms are equivalent sufficiently near the resonance and they are constrained by universal two-body physics.
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The abstract, sentence by sentence
The dark matter annihilation rate at small relative velocities can be amplified by a large boost factor using various mechanisms, including Sommerfeld enhancement, resonance enhancement, and Breit-Wigner enhancement. These mechanisms all involve a resonance near the threshold for a pair of dark matter particles. We point out that if the resonance is in the S-wave channel, the mechanisms are equivalent sufficiently near the resonance and they are constrained by universal two-body physics. The amplified annihilation rate requires a corresponding amplification of the elastic scattering cross section. If the resonance is a bound state below the threshold, it has an increased lifetime that is inversely proportional to the square root of the binding energy. Its spatial structure is that of two dark matter particles whose mean separation is also inversely proportional to the square root of the binding energy.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The dark matter annihilation rate at small relative velocities can be amplified by a large boost factor using various mechanisms, including Sommerfeld enhancement, resonance enhancement, and Breit-Wigner enhancement. | background 1.00 | 0.05 | 0.04 | asserted 0.60 |
| s1 | These mechanisms all involve a resonance near the threshold for a pair of dark matter particles. | background 1.00 | 0.08 | 0.04 | asserted 1.00 |
| s2 | We point out that if the resonance is in the S-wave channel, the mechanisms are equivalent sufficiently near the resonance and they are constrained by universal two-body physics. | contribution 0.68 | 0.82 | 0.82 | asserted 0.91 |
| s3 | The amplified annihilation rate requires a corresponding amplification of the elastic scattering cross section. | result 0.75 | 0.46 | 0.18 | asserted 1.00 |
| s4 | If the resonance is a bound state below the threshold, it has an increased lifetime that is inversely proportional to the square root of the binding energy. | result 0.97 | 0.54 | 0.08 | asserted 1.00 |
| s5 | Its spatial structure is that of two dark matter particles whose mean separation is also inversely proportional to the square root of the binding energy. | result 0.91 | 0.58 | 0.07 | asserted 1.00 |
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The paper
Original abstract
The dark matter annihilation rate at small relative velocities can be amplified by a large boost factor using various mechanisms, including Sommerfeld enhancement, resonance enhancement, and Breit-Wigner enhancement. These mechanisms all involve a resonance near the threshold for a pair of dark matter particles. We point out that if the resonance is in the S-wave channel, the mechanisms are equivalent sufficiently near the resonance and they are constrained by universal two-body physics. The amplified annihilation rate requires a corresponding amplification of the elastic scattering cross section. If the resonance is a bound state below the threshold, it has an increased lifetime that is inversely proportional to the square root of the binding energy. Its spatial structure is that of two dark matter particles whose mean separation is also inversely proportional to the square root of the binding energy.
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References
How the literature uses it
21 arXiv papers cite this in 36 sentences
Papers citing it · 24 sentences without a confident label
Builds on it 1 paper
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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.
Direct detection of dark matter in universal bound states · Introduction · 0.84
Cites it as background 10 papers
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Braaten and Hammer pointed out that the elastic scattering cross section of the dark-matter particles, their total annihilation cross section, and the binding energy and width of a dark matter bound state are all determined by the complex S-wave scattering length [ref] .
Zero-Range Effective Field Theory for Resonant Wino Dark Matter II. Coulomb Resummation · Introduction · 0.85
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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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For Yukawa forces generated by the exchange of a massive particle, the cross sections can be resonantly enhanced by orders of magnitude for particular mass values [ref] , reflecting the universal physics of large scattering length [ref] in the presence of a shallow bound state (or quasi-bound state for higher partial waves [ref] ).
Perturbative Unitarity Violation in Radiative Capture Transitions to Dark Matter Bound States · Introduction · 0.85
What it cites · 20 sentences without a confident label
Compares with 2 papers
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Near threshold, it scales as $σ_rc(k)∼k/(γ^2 + k^2)$, which is in agreement with the E1 term in the radiative capture cross section for a proton$(p)$ and a neutron($n$) into a deuteron($d$) calculated in a low-energy effective field theory for nucleons with large scattering lengths [ref] .
n+p -> d+gamma for Big-Bang Nucleosynthesis · Radiative Capture of Wimps · 0.95
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Finally, we note that a comparison of our result with the previous work of Pospelov and Ritz [ref] is not possible.
Astrophysical Signatures of Secluded Dark Matter · Radiative Capture of Wimps · 0.90
Cites as background 4 papers
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The use of such a resonance to boost the low-energy annihilation rate was proposed by Ibe et al. [ref] and is called Breit-Wigner enhancement.
Breit-Wigner Enhancement of Dark Matter Annihilation · Dark Matter Scattering · 0.92
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Backović and Ralston have emphasized the importance of the widths of particles in dark matter annihilation [ref] .
Limits on Threshold and "Sommerfeld" Enhancements in Dark Matter Annihilation · Universal Relations · 0.81
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Arkani-Hamed et al. increased the interest in these enhancements when they pointed out that a light gauge boson from a hidden sector could explain several possible anomalies in particle astrophysics [ref] .
A Theory of Dark Matter · Dark Matter Scattering · 0.88
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