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Cosmological Structure Formation A Short Course

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The Cold Dark Matter model is the standard paradigm for cosmological structure formation. Structure grows in a hierarchical manner ... Homogeneity and Isotropy ... – PowerPoint PPT presentation

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Title: Cosmological Structure Formation A Short Course


1
Cosmological Structure FormationA Short Course
  • II. The Growth of Cosmic Structure
  • Chris Power

2
Recap
  • The Cold Dark Matter model is the standard
    paradigm for cosmological structure formation.
  • Structure grows in a hierarchical manner -- from
    the bottom-up -- from small density
    perturbations via gravitational instability
  • Cold Dark Matter particles assumed to be
    non-thermal relics of the Big Bang

3
Key Questions
  • Where do the initial density perturbations come
    from?
  • Quantum fluctuations imprinted prior to
    cosmological inflation.
  • What is the observational evidence for this?
  • Angular scales greater than 1 in the Cosmic
    Microwave Background radiation.
  • How do these density perturbations grow in to the
    structures we observe in the present-day
    Universe?
  • Gravitational instability in the linear- and
    non-linear regimes.

4
Cosmological Inflation
  • Occurs very early in the history of the Universe
    -- a period of exponential expansion, during
    which expansion rate was accelerating
  • or alternatively, during which comoving
    Hubble length is a decreasing function of time

5
Cosmological Inflation
  • Prior to inflation, thought that the Universe was
    in a chaotic state -- inflation wipes out this
    initial state.
  • Small scale quantum fluctuations in the vacuum
    stretched out by exponential expansion -- form
    the seeds of the primordial density
    perturbations.
  • Can quantify the amount of inflation in terms
    of the number of e-foldings it leads to

6
Cosmological Inflation
  • Turns out the 70 e-foldings are required to
    solve the so-called classical cosmological
    problems
  • Flatness
  • Horizon
  • Abundance of relics -- such as magnetic monopoles
  • Homogeneity and Isotropy
  • Inflation thought to be driven by a scalar field,
    the inflaton -- could it also be responsible for
    the accelerated expansion (i.e. dark energy) we
    see today?
  • Turns out that angular scales larger than 1º in
    the CMB are relevant for testing inflation --
    also expect perturbations to be Gaussian.

7
The Seeds of Structure
  • Temperature Fluctuations in the Cosmic Microwave
    Background
  • Credit NASA/WMAP Science
    Team (http//map.gsfc.nasa.gov)

8
Temperature and Density Pertubations
  • CMB corresponds to the last scattering surface of
    the radiation -- prior to recombination Universe
    was a hot plasma -- at z1400, atoms could
    recombine.
  • Temperature variations correspond to density
    perturbations present at this time -- the
    Sachs-Wolfe effect

9
Characterising Density Perturbations
  • We define the density at location x at time t by
  • This can be expressed in terms of its Fourier
    components
  • Inflation predicts that ? can be characterised as
    a Gaussian random field.

10
Gaussian Random Fields
  • The properties of a Gaussian Random Field can be
    completely specified by the correlation function
  • Common to use its Fourier transform, the Power
    Spectrum
  • Expressible as

11
Aside Setting up Cosmlogical Simulations
  • Generate a power spectrum -- this fixes the dark
    matter model.
  • Generate a Gaussian Random density field using
    power spectrum.
  • Impose density field d(x,y,z) on particle
    distribution -- i.e. assignment displacements and
    velocities to particles.

12
Linear Perturbation Theory
  • Assume a smooth background -- how do small
    perturbations to this background evolve in time?
  • Can write down
  • the continuity equation
  • the Euler equation
  • Poissons equation

13
Linear Perturbation Theory
  • Find that
  • the continuity equation leads to
  • the Euler equation leads to
  • Poissons equation leads to

14
Linear Perturbation Theory
  • Combine these equations to obtain the growth
    equation
  • Can take Fourier transform to investigate how
    different modes grow

15
Linear Perturbation Theory
  • Linear theory valid provided the size of
    perturbations is small -- ?ltlt1
  • When ?1, can no longer trust linear theory
    predictions -- problem becomes non-linear and we
    enter the non-linear regime
  • Possible to deduce the approximate behaviour of
    perturbations in this regime by using a simple
    model for the evolution of perturbations -- the
    spherical collapse model
  • However, require cosmological simulations to
    fully treat gravitational instability.

16
Next Lecture
  • The Spherical Collapse Model
  • Defining a dark matter halo
  • The Structure of Dark Matter Haloes
  • The mass density profile -- the Navarro, Frenk
    White universal profile
  • The Formation of the First Stars
  • First Light and Cosmological Reionisation

17
Some Useful Reading
  • General
  • Cosmology The Origin and Structure of the
    Universe by Coles and Lucchin
  • Physical Cosmology by John Peacock
  • Cosmological Inflation
  • Cosmological Inflation and Large Scale
    Structure by Liddle and Lyth
  • Linear Perturbation Theory
  • Large Scale Structure of the Universe by
    Peebles
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