BEGIN:VCALENDAR
VERSION:2.0
PRODID:-//linuxsoftware.nz//NONSGML Joyous v1.4//EN
BEGIN:VEVENT
SUMMARY:Dark Matter in Compact Stars
DTSTART:20250925T143000Z
DTEND:20250925T160000Z
DTSTAMP:20260703T131958Z
UID:4c9879fb-dee9-4f62-b3f8-387f509cb15d
SEQUENCE:2
CREATED:20250925T091752Z
DESCRIPTION:Compact stellar objects are promising cosmic laboratories to t
 est fundamental interactions\, in particular they could shed light on the 
 nature of dark matter (DM). DM captured by the strong gravitational field 
 of these stellar remnants transfers kinetic energy to the star during the 
 collision. This together with further DM annihilation in the stellar inter
 ior can have various observational consequences such as the anomalous heat
 ing of old compact stars and compact star destruction for non-annihilating
  DM. We have improved former calculations of the capture and thermalizatio
 n rates in both white dwarfs (WDs) and neutron stars (NSs)\, making little
  approximations about the physics of compact stars. While DM deposits its 
 kinetic energy in the star quite quickly\, for appreciable annihilation he
 ating to be achieved\, capture and annihilation processes should reach a s
 tate of equilibrium. We also revisit the calculation of the capture-annihi
 lation equilibrium timescales in neutron stars. For NSs\, we show that cap
 ture-annihilation equilibrium\, and hence maximal annihilation heating\, c
 an be achieved without complete thermalization of the captured dark matter
  for all types of dark matter - baryon interactions. This includes cases w
 here the scattering or annihilation cross sections are momentum or velocit
 y suppressed in the non-relativistic limit. For scattering cross sections 
 that saturate the capture rate\, we find that capture-annihilation equilib
 rium is typically reached on a timescale of less than a year for vector in
 teractions and 10 thousand years for scalar interactions. For fermionic no
 n-annihilating heavy DM\, we also revisit black hole (BH) formation\, accr
 etion\, and evaporation. We find that previous results on the DM-nucleon s
 cattering cross section for a NS to be destructed by a BH from accumulated
  DM can be relaxed by a few orders of magnitude.
LAST-MODIFIED:20250925T091806Z
LOCATION:DF Seminar Room (2-8.3)\, 2nd floor of Physics Building
URL:http://df.vps.tecnico.ulisboa.pt/pt/eventos/dark-matter-in-compact-sta
 rs/
X-ALT-DESC;FMTTYPE=text/html:<p data-block-key="86pep">Compact stellar obj
 ects are promising cosmic laboratories to test fundamental interactions\, 
 in particular they could shed light on the nature of dark matter (DM). DM 
 captured by the strong gravitational field of these stellar remnants trans
 fers kinetic energy to the star during the collision. This together with f
 urther DM annihilation in the stellar interior can have various observatio
 nal consequences such as the anomalous heating of old compact stars and co
 mpact star destruction for non-annihilating DM.<br/><br/> We have improved
  former calculations of the capture and thermalization rates in both white
  dwarfs (WDs) and neutron stars (NSs)\, making little approximations about
  the physics of compact stars. While DM deposits its kinetic energy in the
  star quite quickly\, for appreciable annihilation heating to be achieved\
 , capture and annihilation processes should reach a state of equilibrium. 
 We also revisit the calculation of the capture-annihilation equilibrium ti
 mescales in neutron stars. For NSs\, we show that capture-annihilation equ
 ilibrium\, and hence maximal annihilation heating\, can be achieved withou
 t complete thermalization of the captured dark matter for all types of dar
 k matter - baryon interactions.<br/><br/> This includes cases where the sc
 attering or annihilation cross sections are momentum or velocity suppresse
 d in the non-relativistic limit. For scattering cross sections that satura
 te the capture rate\, we find that capture-annihilation equilibrium is typ
 ically reached on a timescale of less than a year for vector interactions 
 and 10 thousand years for scalar interactions. For fermionic non-annihilat
 ing heavy DM\, we also revisit black hole (BH) formation\, accretion\, and
  evaporation. We find that previous results on the DM-nucleon scattering c
 ross section for a NS to be destructed by a BH from accumulated DM can be 
 relaxed by a few orders of magnitude.</p>
END:VEVENT
END:VCALENDAR
