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Title: Certificate in Astronomy: Galaxies


1
Certificate in AstronomyGalaxies Quasars
  • Dr Lisa Jardine-Wright
  • Institute of Astronomy, Cambridge University

2
Text Book Chapters
  • Mainly 5 6
  • Also includes elements of 7 8
  • Next 2 lectures include elements that will be
    covered in more detain in Module 4 Cosmology.

3
Lectures 11 12 Galaxy Formation Cosmology
  • A Cosmological Model
  • Cosmic History
  • The standard Big Bang model
  • General Theory of Relativity
  • Big Bang Nucleosynthesis
  • Inflation
  • Observing Galaxy Formation
  • Can we observe galaxies forming?
  • The Universe as a laboratory
  • Theory of Galaxy Formation
  • Monolithic -vs- hierarchical collapse
  • Does light follow mass?
  • Simulations of galaxy formation Ellipticals -vs-
    spirals.

4
Formulation of the Standard Hot Big Bang Model
  • 1915 Einsteins General Theory of Relativity
    meant that we could discuss the evolution of the
    Universe in terms of physically.
  • 1922 Friedmann found solutions to Einsteins
    equations to conclude that the Universe was
    either expanding or contracting.
  • 1929 Hubble observed the recession of galaxies
    due to the expansion of the Universe
  • 1946 Gamov predicted from nucleosynthesis that
    the Universe must begin in a very hot dense phase
    and that the Universe should be filled with
    microwaves.

5
Cosmic History
  • The Universe is split into two broad eras -
    radiation-dominated era and the matter-dominated
    era
  • Before t10-6 s
  • All that could exist under such high temperatures
    and densities was a soup of sub-atomic particles
    and radiation.

6
Cosmic History
  • Series of notable epochs in the evolution of the
    Universe
  • tlt 10-6s Quark soup anti-matter and matter
    annihilate releasing photons of radiation
  • t10-6s Formation of protons and neutrons (p
    same as ionised Hydrogen)

7
Cosmic History
  • Series of notable epochs in the evolution of the
    Universe
  • t lt 1min Formation of atomic nuclei of H, D, He
    some Li (known as Nucleosynthesis)
  • During this epoch radiation scatters of free
    electrons thus the Universe is opaque to us.
  • 400,000yrs gt t gt 15mins The Universe has
    expanded and cooled to allow electrons to join
    with nuclei making atoms (recombination).
  • Number of free electrons reduced and so photons
    no longer collide with electrons decoupling
  • Universe becomes transparent once again (when all
    atomic _at_ 400,000 yrs)
  • Matter domination begins

8
Surface of last scattering
  • The point at which the Universe becomes neutral
    is where radiation no longer scatters of free
    electrons.
  • Thus there is a sphere the surface of which is
    where the radiation last scattered of the free
    electrons.
  • Surface of last scattering

9
The Radiation Cosmic Microwave Background
Radiation
  • The radiation that we have referred to so far is
    the CMBR.
  • Since the epoch of last scattering the radiation
    has not interfered with matter and so provides a
    test bed for the properties of the early Universe.

10
Einsteins General Theory of Relativity
  • Einsteins formulated the field equations
  • Using the field equations we can derive the rate
    of expansion of the universe
  • In a spatially flat universe (K0)

11
Big Bang Nucleosynthesis (BBN)
  • Light elements (D, He, Li) were produced in the
    first few minutes of the Big Bang.
  • 3mins after Big Bang the temperature of the
    Universe rapidly cooled and p and n collided to
    produced D.
  • BBN predicts that of the mass in the Universe
  • 25 He
  • 0.01 D
  • lt0.01 Li
  • These results depend critically on the density of
    baryons at the epoch of nucleosynthesis.
  • The fact that He nowhere exists at gt 23 is
    strong evidence that the Universe went through an
    early hot phase.

12
Problems with the Standard Model
  • Flatness Problem
  • In order for the observed geometry of the
    Universe to be maintained as the Universe expands
    and evolved the conditions in the early Universe
    must be very finely tuned
  • Otherwise the Universe would collapse or expand
    very quickly before any structure could form.
  • Horizon Problem
  • We observe that the Universe is homogeneous and
    isotropic.
  • For this to be the case information must have
    been transmitted to and from all regions of the
    Universe - this is impossible because as the
    Universe expands the information would have to
    travel faster than the speed of light!

13
The Solution Inflation
  • The problems of the standard model arises from
    the fact that in the past the Universe was
    decelerating in its expansion. (velocity
    decreases)
  • Inflation is a phase in the very early Universe
    of extremely rapid expansion
  • After inflation the Universe continues according
    to the standard Hot Big Bang model.

14
The Solution Inflation
  • Flatness Problem
  • The extremely rapid expansion means that (aH)
    increases so O-1? 0.
  • Therefore O ? 1
  • Horizon Problem
  • Regions were causally connected in the period of
    inflation and rapid expansion.

15
Observing Galaxy Formation
  • Ideally we would like to observe galaxies as they
    form and evolve!
  • Problems
  • Time taken for a galaxy to form or evolve many
    100,000s and billions of years.
  • Cannot really predict where a galaxy would form
  • Distant galaxies are extremely faint
  • Solutions?
  • Use the constant speed of light
  • Statistical methods

16
Observing Galaxy Formation
  • What would we like to know?
  • Sizes as a function of time?
  • Brightness as a function of time?
  • And therefore how many stars are being born in
    the past compared with today?
  • Type as a function of time?
  • Distribution of types and how that evolves with
    the Universe?
  • The relation between normal galaxies and active
    galaxies
  • Do all galaxies have supermassive black holes?
  • Are there differences between the galaxies that
    live in clusters and those that exist in the
    field?
  • ..

17
Observing Galaxy Formation
  • Task to find the most distant galaxies in the
    Universe and understand their properties.
  • Naturally there are problems
  • Selection effects
  • Automatically choosing the brightest galaxies
    otherwise we wouldnt be able to see them -
    quasars.
  • Does this mean that all normal galaxies evolve
    from quasars?
  • Or can we just not observe normal galaxies due to
    their low brightness.

18
Brief Theoretical Interlude
  • Theory 1 Monolithic collapse
  • 60 70s
  • Rapid gravitational collapse ? large galaxies ?
    huge bursts of star formation at early epochs
    Galaxies rapidly exhausting their fuel leaving
    behind a collection of old red stars.
  • Hierarchical structure formation.
  • Universe in which smallest mass collapses first
    and merges in to progressively larger structures.

19
Observing Star Formation
  • How do we observe galaxies at high redshifts (z)?
  • Method
  • To investigate galaxies at zgt1, look for expected
    strong features in the spectra of galaxies.

20
Observing High-z Galaxies
  • At very high redshifts the sharp break in
    wavelength at the lyman break is moved into the
    ultra-violet (UV).
  • This method enables us to distinguish between
    nearby extremely red objects and high redshift
    galaxies.
  • If a galaxy is truly distant the image will
    disappear in the UV.

21
UV Dropouts
22
Narrow Band Ly-a Observations
  • SFR of high redshift galaxies will help to
    confirm the current hierarchical theory of
    structure formation.
  • Lots of small, high redshift galaxies of low
    luminosity ? Hierarchical collapse
  • Large galaxies with high SFR ? Monolithic
    collapse
  • Hu, McMahon Cowie have made observations, using
    the 10m Keck Telescope, of a galaxy at z5.74
    (Universe 1 Gyr)
  • To calculate the SFR of this galaxy they used
    narrowband imaging of the Ly-a peak region of the
    spectrum

23
Hu et al. Observations
24
1. CIRPASS
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29
Telescopes Instrumentation
  • Dr Lisa Wright,
  • Astrophysics and Cosmology Back to the Future

30
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35
Galaxy Morphologies
  • Giavalisco et al. presented deep HST images of 19
    Lyman-break galaxies, 6 of which we know have
    2.8ltzlt3.4.
  • They find that light in most of these galaxies is
    concentrated in a central lump. Spheroids
  • However the galaxies are also surrounded by low
    surface brightness gaseous regions, suggesting
    systems in interaction. Hierarchical merging?

36
Galaxy Morphologies
37
Evidence of Hierarchical Merging
38
The quest is on
  • Even though observations have improved hugely
    over the last two decades they still do not
    present us with the definitive answer to galaxy
    formation.
  • What we would like is the distribution of galaxy
    types as we look back in time.
  • Selection effects make this almost impossible to
    investigate.
  • As telescopes continue to improve however we will
    approach the answer.

39
What Do We Understand So Far? Simulating Galaxy
Formation
  • The range of scales that are important in galaxy
    formation makes detailed simulations difficult.
  • Simulations of the formation of elliptical
    galaxies have proved relatively simple compared
    with the formation of disc or spiral galaxies.
    Why?
  • We need to understand in more detail the
    mechanisms of star formation and how early star
    formation in a galaxy affects later star
    formation.

40
Forming Disc Galaxies
  • Simple theoretical model of galaxy formation
  • Dark matter halos provide the potential wells in
    which the material of the galaxy collects and
    collapses.
  • The gas and dust conserves its angular momentum
    during the collapse to a disc. (Fall Efstathiou
    80)
  • Galaxies form from the inside out, thus growing
    with time.
  • Cooling and angular momentum catastrophes.
  • Efficient cooling at early epochs causes the gas
    to collapse into the centres of the dark halos.
    (White Rees 78, White Frenk 91)
  • Gaseous cores subsequently merge and lose angular
    momentum to their surrounding halo. (Navarro,
    Frenk White 95)
  • Disc galaxies which are too small and have too
    little angular momentum. (Navarro Steinmetz 97)

41
Structure Formation Animation
50 Mpc / 155 million lt yr
42
Catastrophe Solutions
  • Need to prevent the gas from collapsing to form
    stars at very early epochs when the dark matter
    halos are still experiencing many major mergers.
  • Prevent all the gas from cooling by heating the
    reservoir.
  • E.g. Supernovae and supernovae driven winds
  • Maybe we need to tweak the cosmological model
  • Warm dark matter
  • Artificially suppress star formation

43
Dark Matter
  • The temperature of the dark matter sets a lower
    limit on the mass of the first objects to form.
  • Initially hot dark matter in the form of
    neutrinos was favoured. The smallest structures
    that are able to form in a universe of hot dark
    matter is 16 Mpc (3 million lt yrs) across.
  • This led to the idea that galaxies may form from
    large, super-cluster size structures. Galaxy
    formation theory 1.
  • Alternatively in a cold dark matter universe the
    first structures to form are smaller than the
    size of observed galaxies and so galaxies form
    from the mergers of smaller objects
  • Galaxy formation theory 2.

44
Dark Matter and Fluctuations
Galaxy Halo Scales
45
Our Simulation Details 1(Wright, Efstathiou
Eke)
  • Cosmology
  • ?m 0.3, ?? 0.7,
  • H0 65 kms-1Mpc-1,
  • Artificially suppress cooling until z1.
  • Simple (though unrealistic) model of stellar
    feedback.
  • Provides a scheme to test numerical effects on
    the formation of the galaxy.
  • Star formation criteria
  • Gaseous region has to be collapsing
  • ?crit gt 7 x 10-23 kgm-3

46
Our Simulation Details 2
  • Lbox 5 Mpc NDM Ngas 583195112
  • ? Mgas 9 x 106 M
  • ? Spatial resolution lt 1 kpc
  • Using 40 GRAPE 3-A processors and Sun
    workstation,
  • CPU time 3 months, z 24 ? z 0.36
  • Currently only 1 simulation in sample.
  • 5 Simulations at resolution, NDM Ngas 503
  • 25 Simulations at resolution, NDM Ngas 343

47
The GRAPEs
  • The IoA grape system 5 GRAPE 3A boards each
    containing 8 processors 40 processors.
  • GRAPE (GRAvity PipE) chips are hardwired to
    calculate a plummer gravitational force law
  • Calculates the forces on 40 particles by up to
    131,072 in any one function call.
  • GRAPE returns forces, potentials and neighbour
    lists.

48
The Story So Far Spiral Galaxies
49
Disc Galaxy Formation Simulation
50
Numerical Comparisons
51
The Future
  • Masses of distant galaxies are a key piece of
    information required to tie together observable
    luminous matter and simulated dark matter.
  • One of the other challenging aspects of deducing
    the history of galaxies is establishing the
    evolutionary links between samples of galaxies
    observed at different epochs
  • Galaxy morphologies
  • Chemical contents
  • Although computing power and star formation
    mechanisms may improve our current theoretical
    models, large gains will be achieved in
    observational astronomy and the development of
    the next generation of telescopes.
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