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Russell Johnston Dept of Physics and Astronomy University of Glasgow.

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Russell Johnston Dept of Physics and Astronomy University of Glasgow
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Page 1: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Russell Johnston

Dept of Physics and AstronomyUniversity of Glasgow

Page 2: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Edwin Hubble

Page 3: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hubble measured the shift in colour, or wavelength, of the light from distant galaxies.

Galaxy

Page 4: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hubble measured the shift in colour, or wavelength, of the light from distant galaxies.

Galaxy

Laboratory

Page 5: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Wavelength

Energy

Spectrum of a nearby galaxy

Spectrum of a Distant Galaxy

Page 6: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hubble’s Law: 1929Hubble’s Law: 1929

Distant galaxies are receding from us with a speed proportional to their distance

Page 7: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Spacetime is expanding like the surface of a balloon.

As the balloon expands, galaxies are carried farther apart

Page 8: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Although Hubble got the expansion law correct, his measurement of the current rate of expansion was quite wrong, and took many decades to correct.

Page 9: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Measuring the Hubble constant was a key project of the Hubble Space Telescope

Page 10: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

More recently we have extended the Hubble diagram to great distances, using e.g. Supernovae….

Region probed by

Hubble’s data

Page 11: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

redshift

‘Speeding up’ model

‘Slowing down’ model

Models with different shapes

Hubble’s law for nearby supernovae

mea

sure

of

dist

ance

….This has led to a remarkable discovery:The expansion of the Universe is speeding up!

Page 12: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

What is driving the cosmic acceleration?…What is driving the cosmic acceleration?…

Page 13: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 14: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Around Galaxies

0

50

100

150

200

250

300

0 20 40 60 80

Distance from the Galaxy Centre (kpc)

Orb

ital v

eloc

ity (

km/s

)

Typical size of galaxy disk

Page 15: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

What we seeWhat we see

What is really there.

Page 16: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

We can also measure the redshifts of many galaxies.

We call this a redshift survey.

Redshift surveys can tell us many useful things:

• How galaxies cluster in space

• How galaxies evolve in time

• Different types of galaxy and where (and when) they are found

• How galaxies formed in the first place

• How much dark matter and dark energy…

And

Page 17: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

The First Redshift Surveys• CfA Survey #1 : 1977 - 1982

CfA # 1

• Surveyed a total of 1100 galaxies

• Marc Davis,

John Tonry

Dave Latham,

John Huchra,

• Redshift range: out to z

0.05

Page 18: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Our own Galaxy

de Lapparent, Geller, and Huchra (1986), ApJ, 302, L1

de Lapparent, Geller, and Huchra (1986), ApJ, 302, L1

Page 19: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Filament

Rich cluster

Void?

Page 20: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 21: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

CfA # 2

The First Redshift Surveys• CfA Survey #2 : 1985 -1995• John Huchra &• Surveyed a total of 18,000 galaxies

Margaret Geller

• Redshift range: out to z

0.05 208 Mpc

Page 22: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Redshift surveys (mid-

1980s)

1 Mpc = 3.26 milion light years

1 Mpc = 3.26 milion light years

Page 23: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

The largest structures in LCRS are much smaller thanthe survey size

The size of thestructures issimilar in both samples

LCRS

1995 (LAS CAMPANAS)

Page 24: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

The First Redshift Surveys• IRAS PSCz : 1992 – 1996, 15,000 galaxies• Team originally consisted of around 24 members including:

• Catalogued over 83% of the sky -

Will Sutherland,

Steve Maddox,

Largest full sky survey.

Will Saunders,Carlos Frenk &

Seb Oliver,

Luis Teodoro.

Page 25: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Surveys….

The Next Generation

• Ran from 1998 to 2003.• Used the multifibre spectrograph on the Anglo Australian Telescope. • The survey covered two strips : NGP -

75 10

80 15 SGP -

• Photometry was taken from the APM galaxy catalogue. • Galaxies brighter than

19.45b

m

• Recovered a total of 245,591 redshifts, 220,000 of which were galaxies out to 0.2z

The Two Degree Field Galaxy Redshift Survey

(2dFGRS)

Page 26: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

The Two Degree Field Galaxy Redshift Survey

(2dFGRS)

• 35 collaborators fro UK, Australia and the US.• including: Carlos Frenk, Matthew Colles, Richard Ellis, Ofer Lahav, John Peacock, Will Sutherland…. and these guys:

Keith Taylor

Simon Driver

Karl Glazebrook Nick

Cross

Shaun Cole

Peder Norberg

Warrick Couch

Page 27: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 28: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

The Two Degree Field Galaxy Redshift Survey

(2dFGRS)

Page 29: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

The Two Degree Field Galaxy Redshift Survey

(2dFGRS)

Page 30: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 31: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 32: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

= 100 Mpc diameter

Page 33: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

The Sloan Digital Sky Survey

(SDSS)• Most ambitious ongoing

survey to date.• Began in early nineties and was due to complete in 2008 …. ish

• Uses a dedicated 2.5m telescope on Apache Point, new Mexico and a pair of spectrographs that measure more than 600 galaxy spectra in a single observation.

• Currently on data release 5 which contains 674749 galaxies.

• On completion will have surveyed over 1 million galaxies.• The Survey has over 150 collaborators at 26 institutions

Page 34: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

The Sloan Digital Sky Survey

(SDSS)

Page 35: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

SDSS

CfA

Page 36: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Sloan Digital Sky Survey: The Footprint of the Survey

Page 37: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Area and Size of Redshift Surveys

1.00E+03

1.00E+04

1.00E+05

1.00E+06

1.00E+07

1.00E+08

1.00E+09

1.00E+04 1.00E+05 1.00E+06 1.00E+07 1.00E+08 1.00E+09 1.00E+10 1.00E+11

Volume in Mpc 3

No

of

ob

jec

ts

LCRS

SDSSmain

SDSSred

SDSSabs line

SDSSphoto-z

2dFRCfA+SSRS

SAPMQDOT

2dF

1.00E+03

1.00E+04

1.00E+05

1.00E+06

1.00E+07

1.00E+08

1.00E+09

1.00E+04 1.00E+05 1.00E+06 1.00E+07 1.00E+08 1.00E+09 1.00E+10 1.00E+11

Volume in Mpc 3

No

of

ob

jec

ts

LCRS

SDSSmain

SDSSred

SDSSabs line

SDSSphoto-z

2dFRCfA+SSRS

SAPMQDOT

2dF

Page 38: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

CMBR fluctuations, 380000 years after the Big Bang, are the seeds of today’s galaxies

The pattern of CMBR temperature fluctuations can be used to constrain the background cosmological model and its parameters

Galaxies and Cosmology: the Basic Paradigm

Page 39: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

CMBR fluctuations, 400000 years after the Big Bang, are the seeds of today’s galaxies

The pattern of CMBR temperature fluctuations can be used to constrain the background cosmological model and its parameters

Both the CMBR and present-day galaxy clustering favour :

Galaxies and Cosmology: the Basic Paradigm

CDM

Cold dark matter + non-zero cosmological constant

Page 40: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

CMBR fluctuations, 400000 years after the Big Bang, are the seeds of today’s galaxies

The pattern of CMBR temperature fluctuations can be used to constrain the background cosmological model and its parameters

Both the CMBR and present-day galaxy clustering favour :

Galaxies and Cosmology: the Basic Paradigm

CDM

Cold dark matter + non-zero cosmological constant

The Concordance ModelThe Concordance Model

Page 41: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

CDM

From Lineweaver (1998)

Page 42: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

The cosmological constant now dominates over CDM and

baryonic dark matter (i.e. atoms).

It is not yet clear if is constant, or perhaps evolves with

time.

More generally, is referred to as

‘Dark Energy’.

Page 43: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Dark Energy

Cold Dark Matter

Ato

ms

The cosmological constant now dominates over CDM and

baryonic dark matter (i.e. atoms).

It is not yet clear if is constant, or perhaps evolves with

time.

More generally, is referred to as

‘Dark Energy’.

Page 44: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Dark Energy

Cold Dark Matter

Ato

ms

The cosmological constant now dominates over CDM and

baryonic dark matter (i.e. atoms).

It is not yet clear if is constant, or perhaps evolves with

time.

More generally, is referred to as

‘Dark Energy’.

Unlike ‘normal’ matter, dark

energy is gravitationally repulsive :

it is causing the expansion of the

Universe to accelerate.

Page 45: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Dark Energy

Cold Dark Matter

Ato

ms

The cosmological constant now dominates over CDM and

baryonic dark matter (i.e. atoms).

It is not yet clear if is constant, or perhaps evolves with

time.

More generally, is referred to as

‘Dark Energy’.

Unlike ‘normal’ matter, dark

energy is gravitationally repulsive :

it is causing the expansion of the

Universe to accelerate.

This affects the rate of growth of

cosmic structure, which we can model

via computer simulations

Page 46: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hierarchical clustering:

Galaxies form out of the mergers of fragments: CDM halos at high redshift.

Clusters form where filaments and sheets of matter intersect

140 Mpc

11 Gyr ago

Page 47: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hierarchical clustering:

Galaxies form out of the mergers of fragments: CDM halos at high redshift.

Clusters form where filaments and sheets of matter intersect

140 Mpc

8 Gyr ago

Page 48: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hierarchical clustering:

Galaxies form out of the mergers of fragments: CDM halos at high redshift.

Clusters form where filaments and sheets of matter intersect

140 Mpc

Present day

Page 49: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hierarchical clustering:

Galaxies form out of the mergers of fragments: CDM halos at high redshift.

Clusters form where filaments and sheets of matter intersect

20 Mpc

11 Gyr ago

Page 50: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hierarchical clustering:

Galaxies form out of the mergers of fragments: CDM halos at high redshift.

Clusters form where filaments and sheets of matter intersect

8 Gyr ago

20 Mpc

Page 51: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hierarchical clustering:

Galaxies form out of the mergers of fragments: CDM halos at high redshift.

Clusters form where filaments and sheets of matter intersect

Present day

20 Mpc

Page 52: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hierarchical clustering:

Galaxies form out of the mergers of fragments: CDM halos at high redshift.

Clusters form where filaments and sheets of matter intersect

11 Gyr ago

20 Mpc

Page 53: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hierarchical clustering:

Galaxies form out of the mergers of fragments: CDM halos at high redshift.

Clusters form where filaments and sheets of matter intersect

8 Gyr ago

20 Mpc

Page 54: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hierarchical clustering:

Galaxies form out of the mergers of fragments: CDM halos at high redshift.

Clusters form where filaments and sheets of matter intersect

Present day

20 Mpc

Page 55: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Which simulation model matches the observations?...

Page 56: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Hubble’s tuning fork classification

We see spiral and elliptical galaxies…

Page 57: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 58: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 59: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Morphological Segregation

Nowadays we find few spiral galaxies in rich clusters. This is thought to be because the spiral disks are disrupted by tidal forces…

Page 60: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 61: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

Morphological Segregation

Nowadays we find few spiral galaxies in rich clusters. This is thought to be because the spiral disks are disrupted by tidal forces…

…Conversely, many ellipticals (and some spirals) may have formed from galaxy mergers.

See talk by Bonnie Steves

Page 62: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

A long time ago,

in a galaxy far, far away…

Page 63: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 64: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 65: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 66: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 67: Russell Johnston Dept of Physics and Astronomy University of Glasgow.
Page 68: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 2.0

Light travel time =10.3 billion years

Page 69: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 2.1

Light travel time =10.5 billion years

Page 70: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 2.2

Light travel time =10.6 billion years

Page 71: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 2.3

Light travel time =10.8 billion years

Page 72: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 2.4

Light travel time =10.9 billion years

Page 73: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 2.5

Light travel time =11.0 billion years

Page 74: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 2.6

Light travel time =11.1 billion years

Page 75: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 2.7

Light travel time =11.2 billion years

Page 76: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 2.8

Light travel time =11.3 billion years

Page 77: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 2.9

Light travel time =11.4 billion years

Page 78: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 3.0

Light travel time =11.5 billion years

Page 79: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 3.1

Light travel time =11.6 billion years

Page 80: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 3.2

Light travel time =11.6 billion years

Page 81: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 3.3

Light travel time =11.7 billion years

Page 82: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 3.4

Light travel time =11.8 billion years

Page 83: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 3.6

Light travel time =11.9 billion years

Page 84: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 3.7

Light travel time =11.9 billion years

Page 85: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 3.8

Light travel time =12.0 billion years

Page 86: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 4.0

Light travel time =12.1 billion years

Page 87: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 4.1

Light travel time =12.1 billion years

Page 88: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 4.3

Light travel time =12.2 billion years

Page 89: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 4.4

Light travel time =12.2 billion years

Page 90: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 4.5

Light travel time =12.3 billion years

Page 91: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 4.6

Light travel time =12.3 billion years

Page 92: Russell Johnston Dept of Physics and Astronomy University of Glasgow.

z = 5.0

Light travel time =12.5 billion years


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