2.2 Successes of the standard 2 Background 2 Background

2.1 A brief chronology 

With current observational constraints, the physical state of our Universe, as understood in the context of the standard or Friedmann-Lemaître-Robertson-Walker (FLRW) model, can be crudely extrapolated back to tex2html_wrap_inline2515 seconds after the Big Bang, before which the classical description of general relativity is expected to give way to a quantum theory of gravity. At the earliest times, the Universe was a plasma of relativistic particles consisting of quarks, leptons, gauge bosons, and Higgs bosons represented by scalar fields with interaction and symmetry regulating potentials. It is believed that several spontaneous symmetry breaking (SSB) phase transitions occured in the early Universe as it expanded and cooled, including the grand unification transition (GUT) at tex2html_wrap_inline2515 seconds after the Big Bang in which the strong nuclear force split off from the weak and electromagnetic forces (this also marks an era of inflationary expansion and the origin of matter-antimatter asymmetry through baryon, charge conjugation, and charge + parity violating interactions and nonequilibrium effects); the electroweak (EW) SSB transition at tex2html_wrap_inline2519  s when the weak nuclear force split from the electromagnetic force; and the chiral or quantum chromodynamic (QCD) symmetry breaking transition at tex2html_wrap_inline2521  s during which quarks condensed into hadrons. The most stable hadrons (baryons, or protons and neutrons comprised of three quarks) survived the subsequent period of baryon-antibaryon annihilations, which continued until the Universe cooled to the point at which new baryon-antibaryon pairs could no longer be produced. This resulted in a large number of photons and relatively few surviving baryons. A period of primordial nucleosynthesis followed from tex2html_wrap_inline2523 to tex2html_wrap_inline2525  s during which light element abundances were synthesized to form 24% helium with trace amounts of deuterium, tritium, helium-3, and lithium.

By tex2html_wrap_inline2527  s, the matter density became equal to the radiation density as the Universe continued to expand, identifying the start of the current matter-dominated era and the beginning of structure formation. Later, at tex2html_wrap_inline2529  s ( tex2html_wrap_inline2505 years), the free ions and electrons combined to form atoms, effectively decoupling the matter from the radiation field as the Universe cooled. This decoupling or post-recombination epoch marks the surface of last scattering and the boundary of the observable (via photons) Universe. Assuming a hierarchical Cold Dark Matter (CDM) structure formation scenario, the subsequent development of our Universe is characterized by the growth of structures with increasing size. For example, the first stars are likely to have formed at tex2html_wrap_inline2533 years from molecular gas clouds when the Jeans mass of the background baryonic fluid was approximately tex2html_wrap_inline2535 , as indicated in Figure 1. This epoch of pop III star generation is followed by the formation of galaxies at tex2html_wrap_inline2537 years and subsequently galaxy clusters. Though somewhat controversial, estimates of the current age of our Universe range from 10 to 20 Gyrs, with a present-day linear structure scale radius of about tex2html_wrap_inline2539 Megaparsecs, where h is the Hubble parameter (compared to 2-3 Megaparsecs typical for the virial radius of rich galaxy clusters).

  

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Figure 1: Schematic depicting the general sequence of events in the post-recombination Universe. The solid and dotted lines potentially track the Jeans mass of the average baryonic gas component from the recombination epoch at tex2html_wrap_inline2443 to the current time. A residual ionization fraction of tex2html_wrap_inline2445 following recombination allows for Compton interactions with photons to tex2html_wrap_inline2447 , during which the Jeans mass remains constant at tex2html_wrap_inline2449 . The Jeans mass then decreases as the Universe expands adiabatically until the first collapsed structures form sufficient amounts of hydrogen molecules to trigger a cooling instability and produce pop III stars at tex2html_wrap_inline2451 . Star formation activity can then reheat the Universe and raise the mean Jeans mass to above tex2html_wrap_inline2453 . This reheating could affect the subsequent development of structures such as galaxies and the observed Lyman-alpha clouds.



2.2 Successes of the standard 2 Background 2 Background

Computational Cosmology: from the Early Universe to the Large Scale Structure
Peter Anninos
http://www.livingreviews.org/lrr-2001-2
© Max-Planck-Gesellschaft. ISSN 1433-8351
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