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Physical Cosmology 2011/2012
Lecture 2
• Galaxies and galaxy clusters astracers of cosmic structure
• Hubble expansion
• CMB basics
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
Galaxies and galaxy clusters as tracers of cosmic structure
galaxies: 108-1011 starsplus dark matterplus diffuse gas
~ 1 - 60 kpc
1kpc = 3.08 x 1019 m
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
Hubble sequence of galaxies
elliptical galaxies
spiral galaxies
barred spirals
“Early” types “Late” types
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
Galaxy clusters
30 - 1000 galaxies
plus hot gas (107-108 K)plus dark matter
bright X-ray sources
~ 1-5 Mpc
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
SDSS survey
1 million galaxyspectra
100,000 QSOspectra
SDSS = SloanDigital SkySurvey
http://www.sdss.orghttp://www.sdss.org
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
blue red
I-ve v +ve v
Doppler effect and velocities
Tc
T period
wavelength
TT
v
cc
z
vv
Get same result from specialrelativity in the limit v<<c
Classical:
I
x
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
The 2dF survey
250 000 galaxyspectra
25 000 QSOspectra
2dF = twodegree field
www.aao.gov.au/2dfwww.aao.gov.au/2df
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
All but some of the closest galaxies have redshifted spectra.
The “recession” velocity increases linearly with distance
dHv Hubble’s law
For a homogeneous Universe this means expansion.
As the Universe expands it cools Hot Big Bang
Hubble flow peculiar velocity
v
d
pecvv dH
Mpc10vpec ddH
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
The Expansion of the UniverseThe expansion of the universe is described by Hubble’s law
)()(
)()(
)(
1)()()(
00 tHnowHH
trdt
tdR
tRtrtHtv
where R(t) is a dimensionless scaling factor
)(
)()(
0tr
trtR
H0 ~ 70 km/sec/Mpc is the Hubble constant. The dimensionlessHubble constant h is defined as
100/0Hh
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
Hubble’s Original Diagram
redshift
standard candleapparent mag
Hubble estimatedH0~500 km/s/Mpc
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
Cosmological redshift:
RT
1 For radiation temperature scales
inversely with the scale factor
em
obs
em
obs
em
obs
em
obs
factorscale
const1
R
R
T
T
R
TR
Rz
obs
em
R
R
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
4rad,0
4
0rad,0rad 1
)()( z
tR
Rt
At high redshift/early times the Universe was radiation-dominated.
Radiation and matter energy density were equal at:
30001rad,0
mat,0eq
z
at z =0:
3144rad Jm107
CMB
2 Taccontributionfrom relativisticneutrinos
65.0,3.0forJm102 mat310
mat2 hc
At present the Universe is “matter-dominated”.
radiation constant
3mat,0
3
0mat,0mat )1(
)()( z
tR
Rt
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
The Cosmic Microwave Background
• Discovered in 1965 by Penzias and Wilson.
• Has T=2.73 K and is believed to be the radiationpresent in the universe at the time of recombination.
• Was extremely hot (T~109 K) but now appears cold dueto the expansion of the universe.
• Corresponds to the “recombination surface” at aredshift of ~1100.
• Observed temperature fluctuations (~20-70 K) in theCMB are thought to originate from the densityfluctuations at z~1100.
• These density fluctuations should be responsible forobserved large scale structures (galaxies, clusters, etc.)
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
log I (
log
1
2 23bodyblack
kThe
chI
The Cosmic Microwave Background
The CMB dominates the extragalactic background radiationin an Idiagram by two orders of magnitude.
1.36mm220 GHz
radio
Tk2sub-mmfar IR
kThe 3
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
The COBE satellite
http://space.gsfc.nasa.gov/astro/cobe/cobe_home.html
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
COBECMB
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
COBE satellite (1990-1994):
T = 2.728 +/- 0.004 K
best black body known
4
bodyblack
bodyblackmeas
10
I
II
Energy density 4Ta
Compare that to mean density of baryons 31bar m102.2 n
photon density 383
BB
m106.333
Tk
a
Tkn
typical photonenergy
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
10bar 106
n
n
There are 2×109 photons for every baryon.in the Universe.
The Universe has high entropy!
is a fundamental parameter. It is important fornucleosynthesis in the early Universe.
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
Surface of last scattering
The most abundant element, hydrogen, recombined whenT ~ 3000K at zrec ~1100.
The Universe changes from optically thick to optically thinat recombination.
Optical depth for Thomson scattering
23)(
0100
1~
ZXdln e
zl
Te
electrondensity
electronfraction
Thomson cross section
rec4
rec
10
1
zzX
zzX
e
e
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
Us surface of lastscattering atz~1100
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
Measurements of the Anisotropies in the CosmicMicrowave Background (CMB)
• COBE satellite, whole sky, DifferentialMicrowave Radiometer (DMR) 31, 53 and90GHz with 10° resolution.
• WMAP satellite was launched, June 2001, 4year mission. First results came out 2003.
• Boomerang, Antarctic balloon, 90, 150, 240 and400 GHz, 0.2° resolution.
• Planck Satellite, 30-900 GHz, launched 2009.
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
CMB anisotropies from COBE
29 micro-Kelvin fluctuations, 1 part in 100,000
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
Dipole + Galaxy + Cosmicanisotropies. 365 km/sapparent velocity. Pec. vel.of local group ~600 km/s
Cosmic anisotropies
Galaxy + Cosmicanisotropies
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
CMB fluctuationspower spectrum
before 1997.
COBE didn’t haveenough spatial
resolution to detectthe first peak
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
CMB anisotropies from Boomerang
Image is ~40x45 degrees
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
Power spectrumfrom Boomerang
data
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
WMAP measured theCMB with much greaterresolution and sensitivity(one millionth of a degreein temperature) thanCOBE.
WMAP(WilkinsonMicrowaveAnisotropy
Probe)
2011 © University of Cambridge. Not to be quoted or reproduced without permission.
Physical Cosmology 2011/2012
2011 © University of Cambridge. Not to be quoted or reproduced without permission.