1. Cosmology and Dark Matter II: The inflationary Universe Jerry Sellwood

2. Matter-radiation equality Next milestone Very little happens Expansion rate changes

3. Formation of the CMB For the first 300,000 years, the intense radiation kept hydrogen ionized H + + e   H +  Constant scattering of photons –maintains thermal equilibrium with matter –makes the universe opaque But as photons are redshifted, atoms are quite suddenly able to survive The universe quickly becomes neutral and transparent

4. Re-ionization Diffuse gas in the universe did not stay neutral for long First stars and/or quasars emitted enough UV radiation to ionize all the diffuse gas Density is far too low by that time for the ionized gas to be opaque

5. Density of Matter BBN tells us that normal (baryonic) matter  b =  b /  crit = 8  G  b / 3H 0 2  0.04 –In stars in galaxies, gas in galaxies, gas between galaxies in clusters of galaxies –yet most remains undetected – it is believed to fill the universe as very low density ionized gas But galaxies and clusters of galaxies contain much more mass that emits no light

6. Galaxy rotation curves Measure speed of gas using Doppler shift Constant circular speed observed, whereas prediction from visible matter decreases Large mass discrepancy → “dark matter halo” Mass in dark matter (at 30kpc)  4  mass in stars & gas

7. Coma cluster of galaxies Originally studied by Zwicky in 1930s Galaxies moving much faster than expected More than 50 times as much mass as we would have guessed from the brightness of the galaxies

8. Gravitational light deflections

9. Hot gas in galaxy clusters Chandra data (Grego et al) 0.3 – 10 keV from hot gas (+ 3 point sources) Coincident with a distant galaxy cluster Hot gas is gravitationally confined

10. Dark Matter Some 80% – 90% of the matter in the universe is “dark”. What could it be? –Not regular protons, neutrons & electrons –Does not emit any detectable radiation –Does not feel electromagnetic forces –Does not feel the strong nuclear force –Exerts gravitational forces Most popular guess is that it is made of WIMPs – fundamental particles that we have not yet detected in any other manner

12. An open universe? Our best estimate:  DM  0.25  0.05 BBN gave us  b  0.04 Total matter density is therefore  M  0.3  crit No other matter known Seems to imply that we live in an open universe, that will expand forever

13. The Hot Big Bang Successfully accounts for: –Uniform expansion – Hubble’s law –Relic radiation now cosmic microwave background fills all space almost perfectly isotropic –76% hydrogen + 24% helium set up in the first 3 minutes But 4 serious problems with this beautiful picture were apparent by the late 1970s

14. Horizon Problem

15. Uniform temperature of CMB At the time the radiation was emitted, the past light cone of matter in region A did not overlap with that from region B Why are the temperatures the same to 1 part in 10 5 ? Why are they chemically homogeneous Apparently violates causality

16. Flatness problem Recall Friedmann’s equation above –1 st term on RHS decreases as a - , where  =3 for dust,  =4 for radiation –2 nd term on RHS decreases as a -2 a has increased by 10 10 since BBN Why is first term not negligible now? 1–  was no more than 10 -20, but not zero! How did it start out so finely balanced?

17. Structure problem What caused galaxies and clusters of galaxies to form? Surveys reveal a clustering hierarchy –on scales that were larger than the horizon at much earlier times How were the seeds of this frothy structure sowed?

18. Monopole problem Unified gauge theories may predict the existence of one or more stable, superheavy relic particles – e.g. magnetic monopoles They should have been formed in abundance and survived Why is the universe today not dominated by such heavy relics?

19. Inflation Solution is Inflation If the  term dominates, then the scale factor a(t) grows exponentially (recall aH = da/dt) A non-zero  implies a constant energy density   = c 2  /8  G, generally interpreted as “false vacuum” or a scalar field Postulate a large   for a short period in the early universe Long enough for a to increase by  e 100

20. Solves all 4 problems Horizon: Regions of the universe that were close enough to have become homogeneous are now far apart causality is not violated Note that this does not imply superluminal motion

21. Solves all 4 problems Flatness: radius of curvature increases by  e 100, making the universe flat to a very good approximation Monopole: If inflation occurs after the heavy relics have formed, their density is diluted by  e 300

22. Structure Problem Quantum fluctuations during inflation cause tiny variations in the energy density Normally they are short-lived But during inflation, fluctuations on scales close to that of the local horizon get carried outside the horizon and become “frozen in” Random variations about the mean energy density of a flat universe Therefore known as “curvature fluctuations” Re-enter the horizon later