Lecture 24
May 6, 2008
Evidence for the Big Bang
Key Concepts:
- What evidence do we have for the Big Bang?
- What is cosmic microwave background radiation?
- What does it look like?
- What does it tell us?
- What is the thermal history of the universe?
- What is Big Bang nucleosynthesis? (Where did all this stuff come from?)
Cosmic Microwave Background (CMB) Radiation
- The Hubble expansion implies that the universe was ever smaller in the earlier times.
- Smaller volume means higher density of matter and energy.
- The universe was extremely hot at one point, and there must be observable effects! (a smoking gun?)
- The question is "what should one look for?"
- How hot was it?
- What does this glow of hot universe look like?
- When did this light glow start?
- How hot does it appear now?
- Where would you look?
The Discovery
What does the Cosmic Background look like?
_
- Blackbody radiation from a 2.73 K thermal body.
- Smooth and flat to one part in 100,000.
- It is seen in every direction -- Olbers' paradox realized!
What is the Cosmic Background Radiation?
- Transition from radiation-dominated to matter-dominated universe
- mass density: ρm = M/V (ρc ~ 10-29 g/cm3)
- radiation density: ρr = aT4/c2 (ρr = 6.5 x 10-34 g/cm3 for T = 2.7K)
- looking back in time, mass density increases as ρm ∝ (R0/R)3
- looking back in time, radiation density increases as ρr ∝ (R0/R)4 - an extra factor of R from Hubble expansion on radiation temperature T
- ρr/ρm ∝ R0/R
- ρr/ρm ~ 10-3 now, but
ρr/ρm ~ 1 when R0/R ~ 1000 (or 1+z ~ 1000)
==> Universe was radiation-dominated at z > 1000
- Marks an important transition from fully ionized universe to
formation of atoms about 400,000 years ago (transition from opaque to transparent to radiation -- e.g., watch the movie of the water freezing rapidly!)
- A departure from perfect uniformity is present, seeding
the future growth of structures like galaxies. (Why?)
The Tests of the Big Bang: The CMB by the COBE and WMAP
- Discovery of the Cosmic Microwave Background
- Why study the Cosmic Microwave Background?
- The Origin of the Cosmic Microwave Background
- Surface of Last Scattering
History of Matter and Radiation in the Early Universe
Starting from the beginning...
- t < 10-43 sec (the "Planck Era"): current understanding of physics does not work, and we need a better theory of gravity.
- t < 10-38 sec (T > 1029 K; the "GUT Era"): all forces were unified to a single GUT force
- t < 10-10 sec (T > 1015 K; the "Electroweak Era"): electromagnetic and weak forces still combined
- t < 0.001 sec (T > 1012 K; the "Particle Era")
- at T > 1012K, the creation and destruction of baryon-antibaryon pairs were in thermal equilibrium the ambient radiation field.
- quark-antiquark annihilation at t ~ 10-6 sec (T ~ 1013 K) -- asymmetry in weak force produced slightly more quark than anitquark (one in a billion)
- t < 3 minutes (T > 109 K; the "Era of Nucleosynthesis"
- at T < 1010K (a few seconds after the BB), electron-positron annihilation begins. By a few 10s of seconds later, all positrons are gone, and electron neutrinos free-stream ("cosmic neutrino background" at ~2K)
- Cosmic Neutrino Background
- neutron ("beta") decay becomes important as electron and antineutrinos with enough energy are disappearing (half-life of 10 minutes)
- more on nucleosynthesis below.....
- t < 400,000 years (T > 3000 K): The Era of Nuclei
- to the present day (T > 2.7 K): The Era of Atoms and Galaxies
Big Bang Nucleosynthesis ("Roasting Beans with Lightning")
- slightly different from nuclear fusion in stars
- Quiz 24C: why is a proton-neutron collision easier/faster than a proton-proton collision?
- "Goldilocks and Three Bears":
- too hot (more than 1013 K), then no nucleons (protons, electrons, neutrons)
- too cold (less than 107 K), then no fusion
- just right, then H, He, Li, Be, B, ....
- Q: why didn't heavier elements like iron, gold, or uranium form then?
- Relative amount of "first elements" depends on matter density (why is that?)
- Q: how does one measure the relative amount of "first elements"?
Web Resources on Cosmology
Reading assignment for next lecture: Unit 81 & 82