Primordial Black Hole Dark Matter KEK / Sokendai / Kavli IPMU Kazunori Kohri (郡 和範)
Primordial Black Hole Dark Matter
KEK / Sokendai / Kavli IPMU
Kazunori Kohri(郡 和範)
Why PBHs?
LIGO and Virgo have detected gravitationalwave signals from 30 M◉Binary Black Holes
https://www.youtube.com/watch?v=1agm33iEAuo
GW150914 and its merger rates for 30 Msolar masses BBH
M. Sasaki, T. Suyama, T. Tanaka and S. Yokoyama (2016).A 3-body effect is important for the BBH formations
fraction to CDM (ffraction)
Rate
of
GW15
0914
10-1010-910-810-710-610-510-410-30.01
0.1
1
10
1015 1020 1025 1030 1035 1040 1045 1050 1055
10-15 10-10 10-5 1 105 1010 1015 1020
SN
HSC
K
E
M
O
IRS
S1 Eri
WBGC
G
DH
DF
CMB
IL
XB
PA
GWLy
LSS
GW2
n/p
GGBEGB
V
CMB
f(M)
M [g]
M/M
Upper bounds on the fraction to CDMf P
BH=Ω
PBH/Ω
CDM
MPBH
Carr, Kohri, Sendouda, J.Yokoyama (2020)
30M⊙
GWs
10−5M⊙
OGLE
104.5M⊙
Seed ofSMBH
Gam
ma-
ray/
CMB
GravitationalLensing Accretion Disk
and CMB
LIGO
2nd GW
Acoustc rehearing CMB µ- distortion
Mass in gram
1017gDM
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
Primordial Black Hole (PBH)• Large perturbation at small scales
was produced by Inflation at around > 10-36 second
2020/10/13 Kazunori Kohri (KEK/Sokendai)
Conditions for a PBH formation in Radiationdominated (RD) Universe
• Gravity could be stronger than pressure
Horizon size = H-1 = (k/a)-1
A fluctuation with the wave number k
δ > δc ~ p / ρ ~ cs2 = w = 1 / 3
Black Hole
A closed universe immediatelycollapsing into a BH
Harada,Yoo and KK (2013)
Zel’dovich and Novikov (1967), Hawking (1971), Carr (1975)
δ
Typical quantities of PBHs in RD• Mass (horizon mass =ρ(tform) H(tform)-3 )
• Fraction to CDM
M
PBH~ M
pl2 t
from~
Mpl3
T 2form
~ 1015 gT
form
3× 108GeV
⎛
⎝⎜⎜
⎞
⎠⎟⎟
−2
~ 30M⊙
Tform
40MeV
⎛
⎝⎜⎜
⎞
⎠⎟⎟
−2
ffraction ⌘⌦PBH⌦CDM
⇠ 108✓MPBH30M�
◆�1/2 pP⇣ exp
� 118P⇣
�
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
P⇣ ⇠< ⇣2 >⇠< �2 >⇠< (�T/T )2 >
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
Curvature perturbation Pζ
KK and T.Terada, 2018
Am
plit
ude
of c
urva
ture
pert
urba
tion
wave number k = p x a
Planck (2015)
at 68% C.L.
For inflation modelswith a big running,see Kohri, Lin Lyth(2008)
P⇣ ⇠< ⇣2 >⇠< �2 >⇠< (�T/T )2 >
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
100 % Dark Matter by PBHs with1017 g masses
KK and T.Terada, 2018
Pulsar timingfor 2nd GW
µ-distortionof CMB
T=TR
The NANOGrav 12.5-year Data Set:Search For An Isotropic Stochastic Gravitational-Wave Background
2020/10/13 Kaz Kohri (KEK)
Zaven Arzoumanian, et al, The NANOGrav Collaboration, arXiv:2009.04496
γ = 3 – 2α = 5 – β
Secondary gravitational wave (GW) nonlinearly-induced by large
curvature perturbation Pζ• Energy density of GWs
Relevant when Pζ >> tensor to scalar ratio r
scalar x scalar modes
⌦GW,c(f) =1
12
✓f
2⇡aH
◆2 Z 1
0dt
Z 1
�1ds
"t(t+ 2)
�s2 � 1
�
(t+ s+ 1)(t� s+ 1)
#2
⇥ I2 (t, s, k⌘c)P⇣✓(t+ s+ 1)f
4⇡�
◆P⇣
✓(t� s+ 1)f
4⇡
◆
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
NANOGrav12.5yr and solar mass PBHs
2020/10/13 Kaz Kohri (KEK)
K. Kohri and T. Terada, arXiv:arXiv:2009.11853
MPBH ⇠ O(1)M�✓
k
107Mpc�1
◆�2⇠ O(1)M�
✓5⇥ 10�9Hz
f
◆2
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
- - - - -×-
× -× -
× -× -
× -× -
PBH+
GW
ffraction ⌘⌦PBH⌦CDM
⇠ 108✓MPBH30M�
◆�1/2 pP⇣ exp
� 118P⇣
�
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
⌦GW,c(f) =1
12
✓f
2⇡aH
◆2 Z 1
0dt
Z 1
�1ds
"t(t+ 2)
�s2 � 1
�
(t+ s+ 1)(t� s+ 1)
#2
⇥ I2 (t, s, k⌘c)P⇣✓(t+ s+ 1)f
4⇡�
◆P⇣
✓(t� s+ 1)f
4⇡
◆
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
NANOGrav12.5yr and solar mass PBHs
2020/10/13 Kaz Kohri (KEK)
K. Kohri and T. Terada, arXiv:arXiv:2009.11853
MPBH ⇠ O(1)M�✓
k
107Mpc�1
◆�2⇠ O(1)M�
✓5⇥ 10�9Hz
f
◆2
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
2020/10/13 Kaz Kohri (KEK)
NANOGrav12.5yr and solar mass PBHsK. Kohri and T. Terada, arXiv:arXiv:2009.11853
Merger GWs
secondary GWs
fPBH=
Summary
• PBH can be produced by large curvature perturbation ζ ~O(1) at small scales in the early Universe
• PBHs with mPBH >O(10) M◉ : LIGO/Virgo
• PBHs with mPBH ~O(1017)g - O(1020)g : DM
• PBHs with mPBH ~O(10-5) M◉ : OGLE events
• PBHs with mPBH ~O(104) M◉ : seeds of SMBH
• PBHs with mPBH ~O(1) M◉: NANOGrav12.5
Typical quantities of PBHs in RD• Mass (horizon mass =ρ(tform) H(tform)-3 )
• Lifetime
• Hawking Temperature
• Fraction to CDM
M
PBH~ M
pl2 t
from~
Mpl3
T 2form
~ 1015 gT
form
3× 108GeV
⎛
⎝⎜⎜
⎞
⎠⎟⎟
−2
~ 30M⊙
Tform
40MeV
⎛
⎝⎜⎜
⎞
⎠⎟⎟
−2
T
PBH~
Mpl2
MPBH
~ 0.1MeVM
PBH
1015 g
⎛
⎝⎜⎜
⎞
⎠⎟⎟
−1
~ 3× 10−11KM
PBH
30M⊙
⎛
⎝⎜⎜
⎞
⎠⎟⎟
−1
τ
PBH~
M3PBH
Mpl4
~ 4 × 1017 secM
PBH
1015 g
⎛
⎝⎜⎜
⎞
⎠⎟⎟
3
~ 3× 1068yrsM
PBH
30M⊙
⎛
⎝⎜⎜
⎞
⎠⎟⎟
3
f
fraction≡Ω
PBH
ΩCDM
~ β10−18
⎛
⎝⎜
⎞
⎠⎟
MPBH
1015 g
⎛
⎝⎜⎜
⎞
⎠⎟⎟
−1/2
~ β10−8
⎛
⎝⎜
⎞
⎠⎟
MPBH
30M⊙
⎛
⎝⎜⎜
⎞
⎠⎟⎟
−1/2
~ 108M
PBH
30M⊙
⎛
⎝⎜⎜
⎞
⎠⎟⎟
−1/2
Pδ
exp − 118P
δ
⎡
⎣⎢⎢
⎤
⎦⎥⎥