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iSkylab 4

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Title: iSkylab 4


1
iSkylab 4
  • Two rungs of cosmic distance ladder
  • First measure distance to Cepheids with parallax,
    also note their periods
  • Establish period-luminosity relationship as slope
    of luminosity vs period graph (L comes from
    BL/(4p d2)
  • Then observe two other Cepheids in two galaxies,
    determine luminosity from period, distance from
    BL/(4p d2)
  • Redshift gives recessional velocity ? Hubbles
    constant as slope in velocity vs distance plot

2
General Relativity ?! Thats easy!

Rµ? -1/2 gµ? R 8pG/c4 Tµ?
OK, fine, but what does that mean?
  • (Actually, it took Prof. Einstein 10 years to
    come up with that!)

3
Planetary Orbits
  • Sun
  • Planets orbit

4
More General than Special Relativity
  • General Relativity is more general in the sense
    that we drop the restriction that an observer not
    be accelerated
  • The claim is that you cannot decide whether you
    are in a gravitational field, or just an
    accelerated observer
  • The Einstein field equations describe the
    geometric properties of spacetime

5
The Idea behind General Relativity
  • We view space and time as a whole, we call it
    four-dimensional space-time.
  • It has an unusual geometry, as we have seen
  • Space-time is warped by the presence of masses
    like the sun, so Mass tells space how to bend
  • Objects (like planets) travel in straight lines
    through this curved space (we see this as
    orbits), so
  • Space tells matter how to move

6
Effects of General Relativity
  • Bending of starlight by the Sun's gravitational
    field (and other gravitational lensing effects)

7
Assumption Cosmological Principle
  • The Cosmological Principle on very large scales
    (1000 Mpc and up) the universe is homogeneous and
    isotropic
  • Reasonably well-supported by observation
  • Means the universe has no edge and no center
    the ultimate Copernican principle!

8
What General Relativity tells us
  • The more mass there is in the universe, the more
    braking of expansion there is
  • So the game is
  • Mass vs. Expansion
  • And we can even calculate who wins!

9
The Fate of the Universe determined by a single
number!
  • Critical density is the density required to just
    barely stop the expansion
  • Well use ?0 actual density/critical density
  • ?0 1 means its a tie
  • ?0 gt 1 means the universe will recollapse (Big
    Crunch) ? Mass wins!
  • ?0 lt 1 means gravity not strong enough to halt
    the expansion ? Expansion wins!
  • And the number is ?0 lt 1 (probably)

10
The size of the Universe depends on time!
Expansion wins!
Its a tie!
Mass wins!
Time
11
The Shape of the Universe
  • In the basic scenario there is a simple relation
    between the density and the shape of space-time
  • Density Curvature 2-D example Universe
    Time Space
  • ?0gt1 positive sphere closed,
    bound finite
  • ?01 zero (flat) plane open, marginal
    infinite
  • ?0lt1 negative saddle open, unbound
    infinite

12
Back to Expansion of the Universe
  • Either it grows forever
  • Or it comes to a standstill
  • Or it falls back and collapses (Big crunch)
  • In any case Expansion slows down!

Surprise of the year 1998 (Birthday of Dark
Energy) All wrong! It accelerates!
13
Enter The Cosmological Constant
  • Usually denoted ?0, it represents a uniform
    pressure which either helps or retards the
    expansion (depending on its sign)
  • Physical origin of ?0 is unclear
  • Einsteins biggest blunder or not !
  • Appears to be small but not quite zero!
  • Particle Physics biggest failure

14
Triple evidence for Dark Energy
  • Supernova data
  • Large scale structure of the cosmos
  • Microwave background

15
Microwave Background Signal from the Big Bang
  • Heat from the Big Bang should still be around,
    although red-shifted by the subsequent expansion
  • Predicted to be a blackbody spectrum with a
    characteristic temperature of 2.725 Kelvin by
    George Gamow (1948)
  • ? Cosmic Microwave Background Radiation (CMB)

16
Discovery of Cosmic Microwave Background
Radiation (CMB)
  • Penzias and Wilson (1964)
  • Tried to debug their horn antenna
  • Couldnt get rid of background noise
  • ? Signal from Big Bang
  • Very, very isotropic (1 part in 100,000)

17
CMB Heres how it looks like!
Peak as expected from 3 Kelvin warm object
Shape as expected from black body
18
Latest Results PLANCK
  • Measure fluctuations in microwave background
  • Expect typical size of fluctuation of ½ degree
    if universe is flat
  • Result
  • Universe is flat !

19
Experiment and Theory
Expect accoustic peak at l200 ? There it is!
20
Supernova Data
  • Type Ia Supernovae are
  • standard candles
  • Can calculate distance
  • from brightness
  • Can measure redshift
  • General relativity gives us distance as a
  • function of redshift for a given universe
  • Supernovae are further away than
  • expected for any decelerating (standard)
  • universe

21
Pie in the Sky Content of the Universe
5
Dark Energy Dark Matter SM Matter
23
72
  • ?We know almost everything about almost nothing!

22
Properties of Dark Energy
  • Should be able to explain acceleration of cosmic
    expansion ? acts like a negative pressure
  • Must not mess up structure formation or
    nucleosynthesis
  • Does not dilute as the universe expands ? will be
    different of content of universe as time goes
    by

23
Threefold Evidence
  • Three independent measurements agree
  • Universe is flat
  • 28 Matter
  • 72 dark energy

24
Cosmic Inflation
  • Size of the universe suddenly increased
    exponentially

25
Consequences
  • Fluctuations at a tiny
  • fraction of a second when all parts of the
    universe talked to each other (to make sure
    everyone was at the same temperature)
  • Suddenly fluctuations are enlarged
  • Fluctuations become imprinted on CMB, provide
    seeds for large scale structure of universe
    (clups that grow into galaxies)

26
Inflation solves the Horizon Problem
  • How does one side of the universe know what
    temperature the other side is at?
  • It has no way, because light (signal velocity) is
    too slow
  • Need inflation at larger than light speed

27
History of the Universe Hot small ? cold big
  • before 10-43 s ?????? (Planck Era)
  • 10-43 s T1032 K gravity splits from other
    forces
  • 10-43 to 10-35 s Grand Unification era
  • 10-35 s T1028 K Strong force splits from
    others. Epoch of inflation?
  • 10-35 s to 10-10 s Electroweak era
  • 10-10 s T1015 K Electromagnetic force splits
    from others
  • 10-10 to 10-4 s Quark era
  • 10-4 s T1013 K Quarks combine to form protons
    and neutrons
  • 10-4 to 500,000 years Radiation era
  • 180 s (3 minutes) T109 K Protons and neutrons
    combine to form nuclei (mainly Helium,
    deuterium)
  • 500,000 years T3,000 K Nuclei and electrons
    combine to form atoms Decoupling
  • 500,000 years to present Matter era
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