Detecting dark matter made in supernovae
G u s t a v
- Ma
r q u e s
- T
a v a r e s , U n i v e r s i t y
- f
Ma r y l a n d
In collaboration with W. DeRocco, P.W. Graham, D. Kasen and S. Rajendran (arxiv:1905.09284)
Detecting dark matter made in supernovae G u s t a v o Ma r - - PowerPoint PPT Presentation
Detecting dark matter made in supernovae G u s t a v o Ma r q u e s - T a v a r e s , U n i v e r s i t y o f Ma r y l a n d In collaboration with W. DeRocco, P.W. Graham, D. Kasen and S. Rajendran
G u s t a v
r q u e s
a v a r e s , U n i v e r s i t y
Ma r y l a n d
In collaboration with W. DeRocco, P.W. Graham, D. Kasen and S. Rajendran (arxiv:1905.09284)
arxiv: 1709.00688
– Kinetic energy ~ 10-6 mdm < keV
– Kinetic energy ~ 10-6 mdm < keV
– delayed arrival – signal spread
SN1987a was 55 kpc away (~ 150000 years)
F l u x d i l u t e d b y
We computed the flux with a Monte Carlo simulation, but many aspects can be understood analitically using a radial freeze-out approach (assuming static profile)
Rate vs Timescale e.g.
Freeze-out in time Freeze-out in radius
Mean free path vs Size e.g.
Number Sphere RN Energy Sphere RE Scattering Sphere RT
Only one type of interaction Diffusion
The total distance traveled to move λann is enhanced by
Freeze-out condition:
For most of the parameter space: For electron scattering: Large backgrounds from neutrinos
For electron scattering: Large backgrounds from neutrinos For nuclear scattering: With Liquid Xenon targets: Bonus: For most of the parameter space: