Transcript Document

NEUTRINO DECOUPLE as Hot DM
• Neutrinos are kept in thermal equilibrium by the creating
electron pairs and scattering (weak interaction):
   e  e


  e    e
• This interaction freezes out when the temperature drops to
kT~MeV~ rest mass electrons
– Because very few electrons are around afterwards
• Argue that Neutrinos have Relativistic speeds while
freezing out
– kT >> rest mass of neutrinos(~eV)
– They are called Hot Dark Matter (HDM)
– Move without scattering by electrons after 1 sec.
e.g., Neutrons
• Before 1 s, lots of neutrinos and electrons keep the
abundance of protons about equal to that of
neutrons through
– n +   p + e• After 1 s free-moving neutrons start to decay.
– n  p + e- + 
– Argue that presently fewer neutrons in nuclei
than protons
thermal equilibrium number density
• The thermal equilibrium background number
density of particles is given by:
 4 3 
d
p 

g
 3

n 3 
h 0 expE / kT   1
+ for Fermions
- for Bosons
E  m 2c 4  p 2c 2
• Where we have to change to momentum space
and g is the degeneracy factor.
E  c 2 p 2  (m c2 ) 2  cp relativistic cp  mc2
2
1
p
 m c2 
2 m
non relativistic cp  mc2
• As kT cools, particles go from
• From Ultrarelativistic limit. (kT>>mc2)
particles behave as if they were massless

2
kT
4

g
y
dy
 
n 
3  y
c
(
2


)
e 1
 
0
• To Non relativistic limit (kT<< 0.1mc2.) Here we
can neglect the 1 in the occupancy number
3
ne
mc 2

kT

4g
 y2 2
(2mkT )
e y dy
3 
(2) 0
3
2
Number density of particles
(annihilating/creating in a photon bath)
Number Density N =
g
h
3
. o
 4 p 3 

 3

d
E
e
kT
E  c 2 p 2  m 2c 4
1
  0.122 boson 
3
 KT 
 g.
 
 hc 
 g.

(Relativistic)
3
2 2
mc 2
2KT .mc

e KT
3 3
g  2  ,e, p
g 1 

h .c
 0.091 fermion e
Non-Relativistic
Particles Freeze Out
• Freeze-out of equilibrium (relativistic or
non-relativistic) at certain temperature
depending on number density, and crosssection.
• Generally a particle A undergoes the reaction:
A A  
• When the reverse reaction rate is slower than
Hubble expansion rate, it undergoes freezeout.
NA
N ph
A LOWweak interaction
early freeze out while relativistic
Freeze out
A HIGHstrong interaction
later freeze out at lower T
m c2
kT
A general history of a massive particle
• Initially relativistic, dense (comparable to photon
number density),
– has frequent collisions with other species to be in
thermal equilibrium and cools with CBR photon bath.
Freeze-Out
•
Later, Relics Freeze-out of the cooling heat bath because
–
–
–
interactions too slow due to lower and lower density in
expanding universe.
This defines a “last scattering surface” where optical depth drops
below unity.
The number density falls with expanding volume of universe,
but Ratio to photons kept constant.
Number density of
non-relativistic particles to
relativistic photons
• Reduction factor ~ exp(-mc2/kT), which
drop sharply with cooler temperature.
• Non-relativistic particles (relic) become
rarer as universe cools (if maintain coupledequilibrium).
smallest Collision cross-section
• neutrinos (Hot DM) decouple from
electrons (via weak interaction) while still
relativistic kT>Δmc2.
•
Small Collision cross-section
• Decouple at non-relativistic once kT<Δmc2 .
Number density ratio to photon drops steeply with
cooling exp(- Δmc2/kT).
– anti-protons and wimps (Cold DM) etc. decouple (stop
creating/annihilating) while non-relativistic. Abundant
(CDM).
– non-relativistic and combine into lower energy state. n
 H  D He, e  Neutral H. Neutrons/electrons
Rarer than Hydrogen.
• Tc~109K NUCLEOSYNTHESIS (100s)
• Tc~5000K RECOMBINATION (106 years)
(Redshift=1000)
A worked-out exercise
A A  
z
Show at last scattering surface Optical depth  =   v n ph (z)
0
d (1+z)-n/2
~   v (1+z)
dz
0
dz
~  v (1+z)3-n/2 ~  vT 3-n/2 ~ 1 .
z
3
where n=4 for radiation era.
mc 2
Given that Freeze-out fraction  ~ exp(
)
kT
and assume decouple at kT~mc2 /ln(1/ ),
Argue cosmic abundance
 ~  m ~ T -1m /( v) ~ ( v) 1
dt
dz
dz
A summary: Evolution of Number
Densities
of , P, e, 
PP
P

ee
vv
Num Density
N
Nο
P
 R 


 Rο 
H
e
H+
Now
1012
10
9
103
R
Rο
3
109
Energetic Tail of Photon Bath
dN
dh
9
10
KTc
hvc  25KTc
hvc
N   hc   KTc.  hvc 
e

 .O 1
N ph
 KTc 
2
e 25  252
10-9
"Freeze-out" KTc
hvc
25
hv
NB
N ph
# hardest photons
~ # baryons
“Freeze-out”