Annihilating Mini BHs: Difference between revisions

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|Progenitor            = Annihilating Mini BHs
|Progenitor            = Annihilating Mini BHs
|Type                  = Single
|Type                  = Single
|EnergyMechanism        = N/A
|EnergyMechanism        = -
|EmissionMechanism      = N/A
|EmissionMechanism      = -
|LFRadioCounterpart    = N/A
|LFRadioCounterpart    = -
|HFRadioCounterpart    = N/A
|HFRadioCounterpart    = -
|MicrowaveCounterpart  = N/A
|MicrowaveCounterpart  = -
|THzCounterpart        = N/A
|THzCounterpart        = -
|OIRCounterpart        = N/A
|OIRCounterpart        = -
|XrayCounterpart        = N/A
|XrayCounterpart        = -
|GammarayCounterpart    = N/A
|GammarayCounterpart    = -
|GWCounterpart          = N/A
|GWCounterpart          = -
|NeutrinoCounterpart    = N/A
|NeutrinoCounterpart    = -
|References            = https://arxiv.org/pdf/1206.4135.pdf
|References            = https://arxiv.org/pdf/1206.4135.pdf
|Comments              = None
|Comments              = None

Revision as of 07:13, 9 October 2018





Summary Table
Category Progenitor Type Energy Mechanism Emission Mechanism Counterparts References Brief Comments
LF Radio HF Radio Microwave Terahertz Optical/IR X-rays Gamma-rays Gravitational Waves Neutrinos
Void Annihilating Mini BHs Single - - - - - - - - - - - https://arxiv.org/pdf/1206.4135.pdf None

Definitions: LF Radio (3 MHz to 3 GHz); HF Radio (3 GHz to 30 GHz); Microwave (30 to 300 GHz)


Model Description

When a BH evaporates to some critical mass, a fireball of e+− pairs can be created. The relativistic pairs expand into the magnetic field of the surrounding ISM, which, for a sufficiently low mass BH, could produce a emission consistent with an FRB.

Observational Constraints

In this scenario the inferred distance to the Lorimer burst is calculated to be 200 kpc -- far too little, thus making this theory inviable.