Nuclear Dark Matter - Synthesis and Phenomenology
APA
Lasenby, R. (2015). Nuclear Dark Matter - Synthesis and Phenomenology. Perimeter Institute. https://pirsa.org/15030101
MLA
Lasenby, Robert. Nuclear Dark Matter - Synthesis and Phenomenology. Perimeter Institute, Mar. 10, 2015, https://pirsa.org/15030101
BibTex
@misc{ pirsa_PIRSA:15030101, doi = {10.48660/15030101}, url = {https://pirsa.org/15030101}, author = {Lasenby, Robert}, keywords = {Particle Physics}, language = {en}, title = {Nuclear Dark Matter - Synthesis and Phenomenology}, publisher = {Perimeter Institute}, year = {2015}, month = {mar}, note = {PIRSA:15030101 see, \url{https://pirsa.org}} }
I will talk about the physics of models in which dark matter consists of composite bound states carrying a large conserved dark “nucleon” number. The properties of sufficiently large dark nuclei may obey simple scaling laws, and this scaling can determine the number distribution of nuclei resulting from Big Bang Dark Nucleosynthesis. For plausible models of asymmetric dark matter, dark nuclei of large nucleon number, e.g. >~ 10^8, may be synthesised, with the number distribution taking one of two characteristic forms, which interestingly are broadly independent of initial conditions. A possible consequence of these scenarios is alterations to direct detection signals, which may be coherently enhanced (relative to collider signals), and could be modified by new momentum-dependent form factors. Inelastic interactions between dark matter states might also be important in astrophysical settings.