Lecture 23 : Four cosmic puzzles! Four puzzles…

Reading: Chapter 16 oftext (inflation)© Sidney Harris

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I : THE FLATNESS PROBLEM! Universe with a flat geometry is a very

special case…
! Ω = 1 (for standard models)! Ω+Λ = 1 (for models with cosmological constant)! Our universe is almost perfectly flat…
! We measure ΩM = 0.315! CMB results suggest that ΩM+ΩΛ ≈ 1 to within 1
percent or better! (Ωk = -0.0005 +- .07)
! Why are we so close to this special case?
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Its worse than that: Ω changeswith time! Ω= ΩM+ΩΛ! |1-Ω|=|k|c2/[H(t)2R(t)2] eq 16.6- so

if k is not identically zero
! For a matter-dominated Einstein-deSitter universe, |1-Ω|~t2/3! For a radiation-dominated universe,|1-Ω|~t! So, if Ω is close to 1 today, it had tobe much much closer to 1 in the past! 3
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In fact, problem is much worse…
! If Ω ≠ 1, then value changes with cosmic

time…

! If Ω > 1, then it grows larger and larger! If Ω < 1, then it grows smaller and smaller

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! If the universe is approximately flat now, it

had to be very, very flat at early times…

! Ω ≈ 1 now, means Ω (at t = 1s) differed from 1 byless than 1 part in 10-16 !!
! At the Plancks time, Ω differed from 1 by lessthan 1 part in 10-60 !!
! So, very special conditions were needed in theearly universe to give approximate flatness now.
! If the Universe were not nearly flat, we would
not be here…

! If Ω had been much above 1, it would have recollapsedvery early before making galaxies! If Ω had been much below 1, it would have expanded so

rapidly that structures would not have formed! This requires a lot of fine tuning!
! It is known as the flatness problem
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II : THE HORIZON PROBLEM! Concept of the particle horizon:! The sphere surrounding a given point (e.g., the Earth)which is causally connected to that point- remember
Minkowski diagrams from 10 weeks ago?

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! Consider 3 locations in space; A, B and C.
! Lets draw their particle horizons…

! So, in this example, A and B are causally connected to eachother. But C is not causally connected to either A or B at thetime of observation.
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7! Consider the epoch of recombination
!Occurred ~400,000 yrs after big-bang!At that time, particle horizon would beroughly 106 light years across.
!This size-scale at the redshift ofdecoupling (z = 1100) corresponds to anangle of about 1° on the sky…
! So, patches of the CBR that areseparated by more than 1 degree
should not have been in causal contact
at the time of decoupling! This gives the horizon problem…(pg467 in textbook)
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! There were a million causally-disconnected

regions on sky at the time of last scattering! How does the CBR know that it has to be
so uniform across the sky?!

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III : THE STRUCTURE PROBLEM! Structure in the universe (galaxies, clusters of galaxiesetc.) came from inhomogeneities in the early universe! We see those same inhomogeneities in the CMB maps…

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! How did those inhomogeneities get there?
! Why are they just the right magnitude and size toproduce the structures we see today?
! How is it possible to have the same kind of
inhomogeneities spread throughout the whole
universe, despite the lack of causal contact
between different parts of the early universe?
! CMB is statistically the same in all directions! Galaxies, etc., that formed are similar in properties, on

opposite sides of the Universe! This is the structure problem.

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IV : THE RELIC PROBLEM! Analogy: consider the cooling of a liquid (e.g.,water)! Once liquid reaches freezing point…

! Freezing does not occur smoothly and uniformly! Freezing starts at certain locations, and the crystals start

growing.
! When crystals eventually merge to form the solid, there
will be dislocations where the individual crystals meet…
! The process of freezing is called a phasetransition (matter changing from one phase to another).

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Dislocations in steel

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Beer crystals (Bud)...

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http://www.microscopy.fsu.edu/beershots/beerphotos.html

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The atomic structure…

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15! What does this have to do with the Universe?
! Quantum fields related to particles and forces inthe very early universe can undergo phasetransitions (i.e., they freeze).
! As Universe cools…

! The temperature falls to the point where certain phasetransitions can occur! Phase transitions will start at particular points in space andgrow at light speed! Can get dislocations produced in the universe as a resultof different regions meeting

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! This would produce exotic structure called

topological defects…
! Domain walls (2-d sheet-like structures)! Cosmic Strings (1-d string-like structures)! None of these have been seen in the observable universe(good limits from CBR data – strings would gravitationallylens the background)! GUTs predict exotic particles produced at these

domain walls in the early Universe! Look like magnetic monopoles! Never detected… and they dont reveal their presence inany observed phenomena. Limits are very good. These
objects have to be very very very rare.

! The absence of monopoles (and other relics

predicted by particle physics theories) is called therelic problem

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Limitations of the Big Bang Theory! While the Big Bang theory successfully explains the "blackbodyspectrum" of the cosmic microwave background radiation and the originof the light elements, it has significant problems:!
The Flatness Problem:
CMB data has determined the geometry of the universe to benearly flat. However, under Big Bang cosmology, curvature grows withtime. A universe as flat as we see it today would require an extreme finetuning of conditions in the past, which would be an unbelievablecoincidence.
!
The Horizon Problem:
Distant regions of space in opposite directions of the sky are so
far apart that, assuming standard Big Bang expansion, they could never
have been in causal contact with each other. This is because the lighttravel time between them exceeds the age of the universe. Yet theuniformity of the cosmic microwave background temperature tells us thatthese regions must have been in contact with each other in the past.

!

The Monopole/Relic Problem:

Big Bang cosmology predicts that a very large number ofheavy, stable "magnetic monopoles" should have been producedin the early universe. However, magnetic monopoles have neverbeen observed, so if they exist at all, they are much more rarethan the Big Bang theory predicts.

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19Inflation Theory to theRescue! Inflation Theory, developed by Alan Guth, Andrei Linde,
Paul Steinhardt, and Andy Albrecht, offers solutions to these
problems and several other open questions in cosmology.
! It proposes a period of extremely rapid (exponential)
expansion of the universe prior to the more gradual Big Bang
expansion, during which time the energy density of theuniverse was dominated by a cosmological constant-type ofvacuum energy that later decayed to produce the matter andradiation that fill the universe today.

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Inflation Continued! Inflation was both rapid, and strong.
! It increased the linear size of the universe by more than 60 "e-folds",

or a factor of ~1026 in only a small fraction of a second!
! Inflation is now considered an extension of the Big Bang theory since
it explains the above puzzles so well, while retaining the basic
paradigm of a homogeneous expanding universe. Moreover, Inflation
Theory links important ideas in modern physics, such as symmetry
breaking and phase transitions, to cosmology.

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How Does Inflation Solve these Problems?
The Flatness Problem:!

!

Imagine living on the surface of a soccer ball (a 2-dimensional world). It
might be obvious to you that this surface was curved and that you wereliving in a closed universe. However, if that ball expanded to the size ofthe Earth, it would appear flat to you, even though it is still a sphere onlarger scales. Now imagine increasing the size of that ball to astronomicalscales. To you, it would appear to be flat as far as you could see, eventhough it might have been very curved to start with. Inflation stretches
any initial curvature of the 3-dimensional universe to near flatness.

The Horizon Problem:

Since Inflation supposes a burst of exponential expansion in theearly universe, it follows that distant regions were actually much closer
together prior to Inflation than they would have been with only standard Big
Bang expansion. Thus, such regions could have been in causal contact prior toInflation and could have attained a uniform temperature.

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! The Monopole Problem:

Inflation allows for magnetic monopoles to exist as longas they were produced prior to the period of inflation. During
inflation, the density of monopoles drops exponentially, so theirabundance drops to undetectable levels.
! As a bonus, Inflation also explains the origin of structure in

the universe. Prior to inflation, the portion of the universe we
can observe today was microscopic, and quantum fluctuationsin the density of matter on these microscopic scales expandedto astronomical scales during Inflation. Over the next several
hundred million years, the higher density regions condensed
into stars, galaxies and us.

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