academic training lectures rocky kolb fermilab, university of chicago, & cern
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Cosmology and the origin of structure. Academic Training Lectures Rocky Kolb Fermilab, University of Chicago, & CERN. Rocky I : The universe observed Rocky II :The growth of cosmological structure Rocky III :Inflation and the origin of perturbations - PowerPoint PPT PresentationTRANSCRIPT
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Academic Training LecturesRocky Kolb
Fermilab, University of Chicago, & CERN
Cosmology and theCosmology and theorigin of structureorigin of structure
Rocky I: The universe observed
Rocky II: The growth of cosmological structure
Rocky III: Inflation and the origin of perturbations
Rocky IV: Dark matter and dark energy
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Rocky Rocky II: The universe observed: The universe observedRocky Rocky II: The universe observed: The universe observed• Cosmological parameters:
• Power spectrum of large-scale structure:
• Anisotropy of CMB:
0
0
0
0
0
Hubble's constant
deceleration parameter
the cosmic food chain
, , , , , , .....
age of the universe
temperature of the u
i
M B
H
q
t
T
niverse
( )P k
lC
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Theoretical developments (1917-1927)Theoretical developments (1917-1927)• Cosmological principle
• Robertson-Walker metric
• Expansion natural
22 2 2 2 2 2 2 2
2( ) sin
1
0, 1 (flat, positive, negative spatial curvature)
drds dt a t r d r d
kr
k
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Observational developments (1912-1929)Observational developments (1912-1929)
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“… physically, he is a splendid specimen…”“… magnificent physique ….”“… manly …”“… loveable character …”
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University of Chicago 1909 National Champions
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Observational developments (1912-1929)Observational developments (1912-1929)
• Cosmological principle (extragalactic astronomy)
• Universe expands
0
-1 -10
recessional velocity
Hubble's constant = 100 km s Mpc
Luminosity distance
R L
R
L
v H d
v c c
H h
d
z
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Hubble’s Discovery Paper - 1929Hubble’s Discovery Paper - 1929Hubble’s Discovery Paper - 1929Hubble’s Discovery Paper - 1929s -1 -1
0 500 km s MpcH
constant sHubble'
v
0
0
H
dH
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0.72 .03 .07 Freedman et al. (Hubble Key Project)
0.57 .02 Sandage, Tammann, et al.
h
h
Riess et al astro-ph/9410054
Hubble’sdata
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Distance-luminosity relationDistance-luminosity relationDistance-luminosity relationDistance-luminosity relation
2
2
2
2(
defines luminosity distance - "know" , measure
Conservation of energy: flux redshifted:
redshift of energy redshift of time interval:
area of
1 )
(1 )
2L
0 1
LF = L F
4 d
=z
z
a t a t
LF = A
A
0
22 2 2 2 2 2 2
0
0
2
2 2 20
centered on sour
(
ce at time of detection,
( ) 4 ( )1
) (1 4 (
)) (1 ) L
S t
drds dt a t r d A a t r
kr
LF =
ad a t r z
t r z
light from comoving coordinate reaches
us now redshifted by an amo ( )unt 1
r
z
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Field equationsField equationsField equationsField equations
2
2
2
8 expansion rate
3
4 13 deceleration parameter
3
a k G aH
a a a
a G ap q
a a H
......M R w
3(1 )whatever: 1
w
w w wp w w p z
0vacuum: 1 1p w z
4radiation: 3 1 3 1R R Rp w z
3matter: 0 0 1 M Mp w z
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Distance-luminosity relationDistance-luminosity relationDistance-luminosity relationDistance-luminosity relation
0( ) (1 )Ld a t r z 2
2 2 2 2 22
( )1
drds dt a t r d
kr
22 ( ) ( )1
dr dt da
a t H a akr
2 2 2 3 3(1 )0 0(1 )(1 ) (1 ) (1 ) ...w
M wH H z z z
light travels on geodesics2 0ds
20
0 0
3 8
... (1 )
i i
M R w
H G
k
1 1
0 0
2 2 3 3(1 )0 00
( )
1 (1 )(1 ) (1 ) (1 ) ...
r z
wM w
a t H dzdr
kr z z z
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Distance-luminosity relationDistance-luminosity relationDistance-luminosity relationDistance-luminosity relation
0( ) (1 )Ld a t r z 1 1
0 0
2 2 3 3(1 )0 00
( )
1 (1 )(1 ) (1 ) (1 ) ...
r z
wM w
a t H dzdr
kr z z z
Program:• measure via
• input and calculate
( )Ld z 2 / 4Ld L F
i 0( )a t r
20 ( )
L
i
H d z O z
Example: matter + lambda 0 M
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Lu
min
osi
ty /
So
lar
Lu
min
osi
ty
10
9
9
8
10
4 10
1.6 10
6.4 10
Type Ia Supernovae
-20 0 20 40 60days
Type Ia supernova are standard candlesType Ia supernova are standard candlesType Ia supernova are standard candlesType Ia supernova are standard candles
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app
aren
t m
agn
itu
de
[lo
g(d
ista
nce
)]
redshift z
Perlmutter et al. (1998)
Type Ia supernova Hubble diagramType Ia supernova Hubble diagramType Ia supernova Hubble diagramType Ia supernova Hubble diagram
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cosmological constant, …some changing non-zero vacuum energy, … or some unknown systematic effect(s)
MATTER
V
AC
UU
M
maximumtheoretical
bliss
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scal
e fa
cto
r a
time
normal0a
Newton Ga pGa 3Einstein
3 0p
scal
e fa
cto
r a
time
accelerated
030
p
a
vacuumenergy?
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The accelerating universe?The accelerating universe?The accelerating universe?The accelerating universe?• Normal matter slows the expansion of the
universe (deceleration). Gravity is attractive.
• Negative pressure would push apart space.
• “Vacuum energy” (the mass-energy density of
space) is positive, but its pressure is negative.
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cosmological constant, …some changing non-zero vacuum energy, … or some unknown systematic effect(s)
MATTER
V
AC
UU
M
The case for :1) acceleration
maximumtheoretical
bliss
2) large-scale structure
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0.25 0.05 0.25 1 0.25
0.25 0.35 0.70
M M
M
h h
h
2dF data
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cosmological constant, …some changing non-zero vacuum energy, … or some unknown systematic effect(s)
MATTER
V
AC
UU
M
The case for :1) acceleration2) large-scale structure
maximumtheoretical
bliss
3) age of the universe
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13.5 2 Gyr
Chaboyer (2001) H0 =70 M t0 (Gyr)
Flat 1.0 0 9.3
Open 0.3 0
12
Open 0.2 0 14
Flat 0.3 0.7 13.5
Flat 0.2 0.8 15
tt00 : age of the universe : age of the universe• white dwarf cooling
• nucleocosmochronology
• globular cluster evolution
Cayrel (2001)
12.6 3 Gyr
First measurement
of stellar uranium
12.6 3 Gyr
13.5 2 Gyr
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cosmological constant, …some changing non-zero vacuum energy, … or some unknown systematic effect(s)
MATTER
V
AC
UU
M
The case for :1) acceleration2) large-scale structure3) age of the universemaximum
theoreticalbliss
4) flatness= 1= 0.31 0.3 = 0.7
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Flat universeFlat universeFlat universeFlat universe
0 1.03 0.06
Hu
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B B hh QSO 1937-1009
Ly
Tytler Tytler
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galaxy kinematics
x-ray gas lensing
M M
= 1
= 0.3
1 0.3 = 0.7
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Cosmo-illogical constantCosmo-illogical constantCosmo-illogical constantCosmo-illogical constant
Mass density of space:
Who ordered that?
The unbearable lightness of nothing!
30 -310 g cm
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Temperature of the universeTemperature of the universeTemperature of the universeTemperature of the universe
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The cosmic food chain (The cosmic food chain (ii))The cosmic food chain (The cosmic food chain (ii))
Radiation: 0.02%
Visible matter: 0.1%
Neutrinos: 0.1%
Dark neutrons & protons: 9.78%
Dark matter: 30%
Dark energy: 60%
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Observer’s view of the universeObserver’s view of the universe
lumpy (inhomogeneous and anisotropic) full of stars, galaxies, clusters, ….
NGC 6070NGC 6070
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Theorist’s view of the universeTheorist’s view of the universe
smooth (homogeneous and isotropic) full of dark matter (and dark energy)
Actual image of dark matterActual image of dark matter
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• Assume there is an average density
• Expand density contrast in Fourier modes
• Autocorrelation function defines power spectrum
Power spectrumPower spectrumPower spectrumPower spectrum
3exp k
xx ik x d k
2 3 2
20
( )( ) ( )
2k
kx dkx x
k
x
3 2
2 22
( ) ( )2
k
k
kk P k
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• Power spectrum related to rms fluctuations
Power spectrumPower spectrumPower spectrumPower spectrum
1( )( )
R
xk R
sphere of radius R
2 2 N
3 3 N
N
. . . . . . . . . .
trial N
1 1 N
. . . . .
1N N2N N
3N N
2iN N
variance
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Power spectrumPower spectrumPower spectrumPower spectrum
3 2
2 1
2k
k
118 Mpch
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Observer’s Observer’s
view of the view of the
universeuniverse
(fluctuations)(fluctuations)
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Theorist’s Theorist’s
view of the view of the
universeuniverse
(isotropic)(isotropic)
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1 2
1/ 22
( , )lm lm
lm l
T T a Y
a C
Angular correlation function, lC
1 1 1 2 2 2( , ) ( , )T T
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Angular power spectrumAngular power spectrumAngular power spectrumAngular power spectrum
LAST CENTURY
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Angular power spectrumAngular power spectrumAngular power spectrumAngular power spectrum
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Angular power spectrumAngular power spectrumAngular power spectrumAngular power spectrum
expected precision
-1 -101 0 50 km s Mpc
0.9 0.1CDM B
n r H
MAP
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Rocky Rocky II: The universe observed: The universe observedRocky Rocky II: The universe observed: The universe observed• Cosmological parameters:
• Power spectrum of large-scale structure:
• Anisotropy of CMB:
0
0
0
0
0
Hubble's constant
deceleration parameter
the cosmic food chain
, , , , , , .....
age of the universe
temperature of the u
i
M B
H
q
t
T
niverse
( )P k
lC
![Page 44: Academic Training Lectures Rocky Kolb Fermilab, University of Chicago, & CERN](https://reader035.vdocuments.mx/reader035/viewer/2022062409/56814d4f550346895dba826a/html5/thumbnails/44.jpg)
Academic Training LecturesRocky Kolb
Fermilab, University of Chicago, & CERN
Cosmology and theCosmology and theorigin of structureorigin of structure
Rocky I: The observed universe
Rocky II: The growth of cosmological structure
Rocky III: Inflation and the origin of perturbations
Rocky IV: Dark matter and dark energy