22
Cosmology and Dark Matter II: The inflationary Universe Jerry Sellwood

Cosmology and Dark Matter II: The inflationary Universe

Embed Size (px)

DESCRIPTION

Cosmology and Dark Matter II: The inflationary Universe. Jerry Sellwood. Matter-radiation equality. Next milestone Very little happens Expansion rate changes. Formation of the CMB. For the first 300,000 years, the intense radiation kept hydrogen ionized H + + e   H +  - PowerPoint PPT Presentation

Citation preview

Page 1: Cosmology and Dark Matter II: The inflationary Universe

Cosmology and Dark Matter II: The inflationary Universe

Jerry Sellwood

Page 2: Cosmology and Dark Matter II: The inflationary Universe

Matter-radiation equality

• Next milestone

• Very little happens

• Expansion rate changes

Page 3: Cosmology and Dark Matter II: The inflationary Universe

Formation of the CMB• For the first 300,000 years, the intense

radiation kept hydrogen ionizedH+ + 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

Page 4: Cosmology and Dark Matter II: The inflationary Universe

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

Page 5: Cosmology and Dark Matter II: The inflationary Universe

Density of Matter

• BBN tells us that normal (baryonic) matter b = b / crit = 8G b / 3H0

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

Page 6: Cosmology and Dark Matter II: The inflationary Universe

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

Page 7: Cosmology and Dark Matter II: The inflationary Universe

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

Page 8: Cosmology and Dark Matter II: The inflationary Universe

Gravitational light deflections

Page 9: Cosmology and Dark Matter II: The inflationary Universe

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

Page 10: Cosmology and Dark Matter II: The inflationary Universe

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

Page 11: Cosmology and Dark Matter II: The inflationary Universe
Page 12: Cosmology and Dark Matter II: The inflationary Universe

An open universe?

• Our best estimate: DM 0.250.05

• BBN gave us b 0.04• Total matter density is

therefore M 0.3crit • No other matter known• Seems to imply that we

live in an open universe, that will expand forever

Page 13: Cosmology and Dark Matter II: The inflationary Universe

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

Page 14: Cosmology and Dark Matter II: The inflationary Universe

Horizon Problem

Page 15: Cosmology and Dark Matter II: The inflationary Universe

Horizon Problem

• 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 105?

• Why are they chemically homogeneous• Apparently violates causality

Page 16: Cosmology and Dark Matter II: The inflationary Universe

Flatness problem

• Recall Friedmann’s equation above– 1st term on RHS decreases as a-, where =3

for dust, =4 for radiation– 2nd term on RHS decreases as a-2

• a has increased by 1010 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?

Page 17: Cosmology and Dark Matter II: The inflationary Universe

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?

Page 18: Cosmology and Dark Matter II: The inflationary Universe

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?

Page 19: Cosmology and Dark Matter II: The inflationary Universe

Solution is InflationInflation

• If the term dominates, then the scale factor a(t) grows exponentially (recall aH = da/dt)

• A non-zero implies a constant energy density = c2/8G, 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 e100

Page 20: Cosmology and Dark Matter II: The inflationary Universe

Solves all 4 problemsHorizon: 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

Page 21: Cosmology and Dark Matter II: The inflationary Universe

Solves all 4 problems

Flatness: radius of curvature increases by e100, making the universe flat to a very good approximation

Monopole: If inflation occurs after the heavy relics have formed, their density is diluted by e300

Page 22: Cosmology and Dark Matter II: The inflationary Universe

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