2021
DOI: 10.48550/arxiv.2112.09147
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Binary Collisions of Dark Matter Blobs

Abstract: We describe the model-independent mechanism by which dark matter and dark matter structures heavier than ∼ 8 × 10 11 GeV form binary pairs in the early Universe that spin down and merge both in the present and throughout the Universe's history, producing potentially observable signals. Sufficiently dense dark objects will dominantly collide through binary mergers instead of random collisions. We detail how one would estimate the merger rate accounting for finite size effects, multibody interactions, and fricti… Show more

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Cited by 6 publications
(6 citation statements)
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“…along the lines of [70,98,99]. The solitons, as mentioned in section 3.5, could also merge in the late Universe or when they are bounded into halos, which could change their mass distribution [100].…”
Section: Possible Improvements and Extensionsmentioning
confidence: 98%
“…along the lines of [70,98,99]. The solitons, as mentioned in section 3.5, could also merge in the late Universe or when they are bounded into halos, which could change their mass distribution [100].…”
Section: Possible Improvements and Extensionsmentioning
confidence: 98%
“…Exotic compact objects [82] can be considerably lighter than a solar mass and therefore can emit GWs at high frequencies. Examples of such exotic compact objects are boson and fermion stars [82][83][84][85], gravitino stars [86], gravistars [87], and dark matter blobs [88]. In general, the GW waveforms generated by merging exotic compact objects and PBHs are distinct, though this difference is small when the orbital radius is much larger than the spatial size of the merging objects; for simplicity, in our analysis we treat the merging objects as point-like.…”
Section: Sourcesmentioning
confidence: 99%
“…Their potentially high compactness implies that mergers can generate GWs detectable with present GW observatories. Most present work in the literature on BSs focusses on the GW signatures generated during the pre-merger infall or inspiral [69][70][71][72][73] and during the merger phase itself [21,28,[74][75][76][77][78][79][80][81][82][83][84][85][86][87][88][89]; these are, of course, the regimes of most notable interest in the GW observation of neutron-star and black-hole binary coalescences. The main focus of our work, however, is the long-lived post-merger GW emission or afterglow resulting from the merger of two BSs into a single compact but horizon-free remnant; for first explorations of BS coalescences including the relaxation into a non-rotating BS or a hairy BH see [75,79,82].…”
Section: Introductionmentioning
confidence: 99%