1 cosmic inflation and the arrow of time a. albrecht ucd p262 spring 2006
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1
Cosmic Inflation and the Arrow of
Time
A. Albrecht
UCD
P262
Spring 2006
2
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
3
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
4
Inflation:
Try and solve the following puzzles/features of the Standard Big Bang (SBB) universe:
• Flatness
• Homogeneity
• Monopole
• Horizon
I.0 What is Cosmic Inflation?
5
a
1
In the SBB, flatness is an “unstable fixed point”:
At GeVT 1610
or
28
0
10a
a
The “GUT scale”
Require c to 55 decimal places to get
c today
22
2
8
3
a kH
a a
c
23
8c
H
Dominates with time
43 , aa
I.0 What is Cosmic Inflation?
i
6
Gravitational instability: The Jeans Length
I.0 What is Cosmic Inflation?
i
1/ 22
Jeans J s
cR c
G
Sound speedAverage energy density
• Overdense regions of size
collapse under their own weight.
If the size is they just oscillate
JeansR
JeansR
7
SBB Homogeneity:
On very large scales the Universe is highly homogeneous, despite the fact that gravity will
clump matter on scales greater than RJeans
At the GUT epoch the observed Universe consisted of 1079 RJeans sized regions.
The Universe was very smooth to start with.NB: Flatness & Homogeneity SBB Universe starts in highly unstable state.
35 35 210 10 4Univ bh Max UnivS S M
i
I.0 What is Cosmic Inflation?
8
SBB Monopolesi
I.0 What is Cosmic Inflation?
• A GUT phase transition (or any other process) that injects stable non-relativistic matter into the universe at early times (deep in radiation era, ie Ti =1016 GeV) will *ruin* cosmology:
3
4 "
( )( )
( )(
"
)
M i
M i
Normal i
Normal
i iM
Norma
i
l T
i
TT T
TT
TT
T
TT
Monopole dominated Universe
9
t=0
Here & Now
SBB Horizon
1080 causally disconnected regions at the GUT epoch
i
I.0 What is Cosmic Inflation?
0
'( ) '
( ')
t
H
dtd a t dt
a t
Hd
Horizon: The distance light has traveled since the big bang:
10I.0 What is Cosmic Inflation?
The flatness, homogeneity & horizon features become “problems” if one feels one must explain initial conditions.
Basically, the SBB says the universe must start in a highly balanced (or “fine tuned”) state, like a pencil on its point.
Must/can one explain this?
Inflation says “yes”
11
The Basic Tools of Inflation:
Consider a scalar field with:1
( ) ( )2
V L
If ( )V all space and time derivative (squared) terms
Then( ) 0 0 0
0 ( ) 0 0
0 0 ( ) 0
0 0 0 ( )
V
VT
V
V
Which implies p 0d
da
~ Hta e Inflation
w=-1
i
I.0 What is Cosmic Inflation?
12
A period of early inflation gives:
Flatness:2
22
8
3
a kH
a a
a
1
Dominates over & during inflation
33
'H
H
Hconst
V
Homogeneity
At horizon crossing:
510HA suitably adjusted potential will
give :
i
I.0 What is Cosmic Inflation?
1c
Evaluate when k=H during inflation
.const
r m
13
A period of early inflation gives:
Monopoles:
a
1
Dominates over & during inflation (and )
i
I.0 What is Cosmic Inflation?
1
1
1
3
1
3
( )( )
( ) (0
)
M
M HtM
a
aa
a Const a
aa
e
M
Monopoles are erased
~ Hta e
22
2
8
3
a kH
a a
1c
r m
14
Inflation Horizon:
Here & Now
Inflation starts
Inflation ends
i
I.0 What is Cosmic Inflation?
15
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
16
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
17I.1 Successes
Inflation:
• An early period of nearly exponential (“superluminal”) expansion set up the “initial” conditions for the standard big bang
Predictions:
• total=1 (to one part in 100,000 as measured)
• Characteristic oscillations in the CMB power
• Nearly scale invariant perturbation spectrum
• Characteristic Gravity wave, CMB Polarization etc
• etc
18
• total=1
Bennett et al Feb 11 ‘03
WMAP
I.1 Successes
19
• total=1
Bennett et al Feb 11 ‘03
WMAP
I.1 Successes
Tegmark et al
astro-ph/0310723
WMAP Only
WMAP + SDSS
20
• Characteristic oscillations in the CMB power
Adapted from
Bennett et al Feb 11 ‘03
WMAP
“Active” models
Inflation
I.1 Successes
Tem
pera
ture
Pow
er
Angular scale
21
•Nearly scale invariant perturbation spectrum
Bennett et al Feb 11 ‘03
WMAP
I.1 Successes
1 sn
H k
k Ak
22
•Characteristic Gravity wave, CMB Polarization etc
Bennett et al Feb 11 ‘03
WMAP
“Active” models
Inflation
TxE polarization power
I.1 Successes
23
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
Cosmic Inflation and the Arrow of Time
24
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
Cosmic Inflation and the Arrow of Time
25
• Emerging prospects for high precisions tests
|nS’ |
ns
n
|nS’ |B. Gold & AA ‘03
I.2 Future tests
Future Ly-alpha
Generic slow roll inflation
WMAP
1 sn
H k
k Ak
( ) n ...lS S Sn k n n k
/ lnS Sn dn d k
26
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
27
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
28I.3 Theoretical advances
A.A, Davis Meeting on Cosmic Inflation ‘03
29
I) Inflation in the era of WMAP
Great accomplishments and exiting future prospects
For an “snapshot” view the slides at:inflation03.ucdavis.edu
30
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
31
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
32II.1 Introduction
1) The physical (“thermodynamic”) arrow of time
2) Cosmic Inflation
Explained by initial conditions
Explains the initial conditions of the cosmos
Davies ’83 & ’84, Page ’83 (Nature)
Q: How are these two related?
33
Why wonder about arrow of time inflation?
•Understand what we are really trying to accomplish with inflation more solid foundations
•Fun combination of physics ideas
•Evaluate “alternatives to inflation”
II.1 Introduction
•Window on current hot topics
34
• Initial conditions in ”normal Physics”:
- Pose physical question
- Chose initial conditions which best describe “apparatus”
- Calculate and compare with experimental results
• Cosmic Inflation: Explain cosmic initial conditions using physics
Initial conditions play supporting role
Laws of physics play supporting role
Examples:
- Arrow of time
- Choice of vacuum in quantum field theory
II.1 Introduction
35
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
36
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
37
See H.D. Zeh The physical basis of the direction of time
- Macroscopic (or thermodynamic) arrow of time emerges from a combination of:
• Dynamical trends or “attractors”
• Special initial conditions
• Choice of coarse graining
- Despite a completely reversible microscopic world
II.2 Arrow of time basics
NB: Not about “T symmetry”
38
Jeansl l , gravity unimportant)(Taking
Dynamical trends or “attractors”
Special initial conditions
Choice of coarse graining
An Example:
II.2 Arrow of time basics
39
• Recording/Learning
• Harnessing energy (actually “low entropy”)
Key roles of the arrow of time:
II.2 Arrow of time basics
40
Key roles of the arrow of time (cont.):
• Quantum Measurement
Everett same old “thermodynamic” arrow of time
II.2 Arrow of time basics
41
- Macroscopic (or thermodynamic) arrow of time emerges from a combination of:
• Dynamical trends or “attractors”
• Special initial conditions
• Choice of coarse graining
Most Fundamental
Entropy, laws of thermodynamics, counting number of states etc:
-Ways to quantify the above
- “Icing on the cake”
II.2 Arrow of time basics
42
Time 1 Time 2 Time 3
II.2 Arrow of time basics
43
Jeansl l : gravity very importantNow consider
A completely different trend/attractor:
Gravitational Collapse
II.2 Arrow of time basics
44
: gravity very important
Equilibrium under gravitational collapse:
Black Hole
(the state of ultimate collapse)
24bhS M
(Sbh not as well developed as ordinary entropy, but good enough for our purposes as a way to quantify a dynamical trend.)
II.2 Arrow of time basics
Jeansl l
45
The Punch Line:
The thermodynamic arrow of time originates with the very special initial conditions of the cosmos:
The early universe is very homogeneous on scales very far from Eqm. (= black hole)
35 35 210 10 4Univ bh Max UnivS S M
Cosmic Microwave Background uniform to one part in 105
Penrose
II.2 Arrow of time basics
Jeansl l
46
The everyday link to gravitational collapse
II.2 Arrow of time basics
47
The everyday link to gravitational collapse
II.2 Arrow of time basics
48
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
49
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
50II.3 Inflation and the arrow of time
Standard inflation spiel begins:
Cosmological problems of standard big bang:
Universe starts far from dynamical trend:
-Flat
-Homogeneous
-Horizons prevent dynamical explanation
Q: How can this fact be explained?But isn’t starting far from the dynamical trend exactly what is required to explain the arrow of time? And when do we ever explain initial conditions anyway?
51
Warm up 1: Big Bang Nucleosynthesis Prediction of abundances.
Time
Mass
Fra
ctio
n
Species
But doesn’t the answer just depend on the initial state?
Figure: Burles, Nollett, &Turner
II.3 Inflation and the arrow of time
52
Warm up 1: Big Bang Nucleosynthesis: Nuclear Statistical (“chemical”) equilibrium (attractor) erases initial conditions dependence.
Time
Mass
Fra
ctio
n
Eq. Time
Time to species freeze-out
Coarse Graining:
Just ask about mass fractions
II.3 Inflation and the arrow of time
53
Warm up 2: Gas in ice
Ice
Insulator
Ice
Time 1
Insulator
II.3 Inflation and the arrow of time
54
Ice
Insulator
Ice
Time 2
Insulator
Warm up 2: Gas in ice
II.3 Inflation and the arrow of time
55
Ice
Insulator
Ice
Time 3
Insulator
Frozen
Warm up 2: Gas in ice
II.3 Inflation and the arrow of time
56
Internal eqm time << freezing time
Internal eqm. set initial conditions for condensation & final frozen state.
Warm up 2: Gas in ice
II.3 Inflation and the arrow of time
57
End warm up… now the real thing:
II.3 Inflation and the arrow of time
58
Key ingredient:
8G T
Cosmological constant => different gravitational at attractor:
de Sitter space
- Perfectly flat, homogeneous, exponentially expandingProperties of Big Bang initial
state
3dSS
Gibbons & Hawking, See also Bousso
Equivalent to “perfect” potential dominated state
II.3 Inflation and the arrow of time
59
Can be mimicked by a scalar field in a special “potential dominated state”
Inflaton field can turn on and off eff
Inflation: Let the inflaton field turn on and leave it on for *many* de Sitter equilibration times, then decay into ordinary matter.
A standard “big bang” (arrow of time and all) is created.
eff
II.3 Inflation and the arrow of time
60
The Inflaton:
Consider a scalar field with:
1( ( )) ( ) ( ) ( ( ))
2x x x V x
L
If )(V all space and time derivative (squared) terms
Htea ~
Inflation
0a
8 ( )GV
V
Quantum fluctuations
II.3 Inflation and the arrow of time
61
Comparisons:
System Initial Conditions
•Nucleosynthesis
•Slow Freeze
•Inflation
V
Created by early time attractor (eqm)
Created by early time attractor (eqm)
Created by early time attractor (eqm)
II.3 Inflation and the arrow of time
62
Comparisons:
System Initial Conditions
•Nucleosynthesis
•Slow Freeze
•Inflation
V
Created by early time attractor (eqm) in subspace
Created by early time attractor (eqm) in subspace
Created by early time attractor (eqm) in subspace
But driven by non-eqm degree of freedom
Background Spacetime
Out of eqm ice
Special Inflaton field configurationIssues with very small scales!II.3 Inflation and the arrow of time
63
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
64
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
65
Does inflation
-Predict the arrow of time? (Sets up IC’s for Big Bang)
-Depend on the arrow of time? (Requires special initial state of inflaton etc.)
II.4 Implications
66
LABLA
BLABLA
BLABLA
B
Comment on how we use knowledge (“A” word!)
Total knowledge about the universe
Input Theory Output
II.4 Implications
67
LABLA
BLABLA
BLAB
LAB
Comment on the “A” word:
Total knowledge about the universe
Input Theory Output
II.4 Implications
68
LABLA
BLABLA
BLAB
LAB
Comment on the “A” word:
Total knowledge about the universe
Input Theory Output
II.4 Implications
69
LABLA
BLABLA
BLAB
LAB
Comment on the “A” word:
Total knowledge about the universe
Input Theory Output
II.4 Implications
70
LABLA
BLABLA
BLAB
LAB
Comment on the “A” word:
Total knowledge about the universe
Input Theory Output
LABPR
ED
II.4 Implications
71
LABLA
BLABLA
BLAB
LAB
Input Theory Output
LABPR
ED
The best science will use up less here and produce more here
II.4 Implications
72
Q: To what extent should our arrow of time (smooth initial state of Big Bang) best used as INPUT, rather than OUTPUT?
A: The arrow of time (smooth initial state of Big Bang) can NOT be 100% output.
The very nature of the arrow of time requires initial conditions that are not completely generic
II.4 Implications
73
What Role What role inflation?
-Gives package deal: Universe very large, flat, and with particular perturbations (falsifiable!). -Answers Boltzmann’s concerns about typical regions with arrow of time being much smaller and “shorter” then we experience. (inflation as amplifier). [Also modern cosmological version.]
- Answers “How did our Universe come about?”
II.4 Implications
NB: In the spirit of Linde’s “chaotic inflation”
-“Dominant channel” into Big Bang (Uses attractor behavior and exponential volume factors to maximize impact)
74
Rare Fluctuation
II.4 Implications
75II.4 Implications
Boltzmann's “cosmology”:
76II.4 Implications
Boltzmann's “cosmology”:
77II.4 Implications
Boltzmann's “cosmology”:
78II.4 Implications
Boltzmann's “cosmology”:
79II.4 Implications
Boltzmann's “cosmology”:
80II.4 Implications
Boltzmann's “cosmology”:
81II.4 Implications
Boltzmann's “cosmology”:
82II.4 Implications
Boltzmann's “cosmology”:
83II.4 Implications
Boltzmann's “cosmology” appeared to make very strange predictions:
84II.4 Implications
Boltzmann's “cosmology”:
85II.4 Implications
Boltzmann's “cosmology”:
86II.4 Implications
Boltzmann's “cosmology”:
(Boltzmann's brain)
87II.4 Implications
Boltzmann's “cosmology”:
88II.4 Implications
Boltzmann's “cosmology”:
89II.4 Implications
Boltzmann's “cosmology”:
90II.4 Implications
Inflation (**schematic**):
91II.4 Implications
Inflation (**schematic**):
92II.4 Implications
)(V all space and time derivative (squared) terms
V
Inflation (**schematic**):
The “rare fluctuation” is in the inflaton field
93II.4 Implications
Inflation exponentially expands the volume
Reheated regions give big bang
Special package of features predicted by inflation
Inflation (**schematic**):
94
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
95
I) Inflation in the era of WMAP
I.0 What is Cosmic Inflation?
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
III) Conclusions
II) Inflation and the arrow of time
II.1 Introduction
II.2 Arrow of time basics
II.3 Inflation and the arrow of time
II.4 Implications
II.5 Can the Universe Afford Inflation?
Cosmic Inflation and the Arrow of Time
96
Dark energy and Equilibrium
97
Supernova
Preferred by modern data
Amount of gravitating matter
A
mount
of
“anti
gra
vit
y”
matt
er
(Dark
En
erg
y)
Red line: No anti-gravity matter
Mass-Energy of the a Universe made only out of standard model matter
Surprise factor
II.5 Can the Universe afford Inflation?
98
An interesting property of some types of dark energy (including a w=-1 cosmological constant): Formation of an event horizon:
Black Hole Event Horizon (schematic):
Outside observer sees in-falling object take infinite time to reach the horizon (“never reaches the horizon”)
II.5 Can the Universe afford Inflation?
99
An interesting property of some types of dark energy (including the cosmological constant): Formation of an event horizon:
Dark Energy Event Horizon (schematic):
INSIDE observer sees OUT-flying object take infinite time to reach the horizon (“never reaches the horizon”)
2 1S A H
t1t2t3t4……
“de Sitter Space”
II.5 Can the Universe afford Inflation?
100
2 1S A H
“De Sitter Space: The ultimate equilibrium for the universe?
Horizon
Quantum effects: Hawking Temperature
8
3 DE
GT H
II.5 Can the Universe afford Inflation?
101
Rare Fluctuation
A cosmological constant can help realize the “rare fluctuation” cosmology.
II.5 Can the Universe afford Inflation?
102
Rare Fluctuation
A cosmological constant can help realize the “rare fluctuation” cosmology.
II.5 Can the Universe afford Inflation?
The only really physics way to discuss “initial” conditions
103
Concept:
Realization:
“de Sitter Space”
II.5 Can the Universe afford Inflation?
104
Rare Fluctuation
II.5 Can the Universe afford Inflation?
105
Big question:
What is the most likely fluctuation to “give what we see:?:
-Normal Big Bang?
-Inflating Region?
II.5 Can the Universe afford Inflation?
106
The universe spends most of its time in “equilibrium”
The equilibrium state is given by an observer’s “causal patch” in de Sitter space with a very small Λ.
Cosmology given by the appearance of rare fluctuations away from this eqm. state.
Recurrence times/probabilities given by stat mech:
fluct
fluct
SS Sfluct
fluct SR
t eP e
t e
Dyson, Kleban & Susskind (hep-th/0208013)AND AA & Sorbo hep-th/0405270
The basic picture:
II.5 Can the Universe afford Inflation?
107
fluct
fluct
SS Sfluct
fluct SR
t eP e
t e
fluctt
Rt1S
fluctP
= Recurrence time for a particular fluctuation
= Recurrence time for whole system
= Total microstates of system
= Probability of fluctuation
II.5 Can the Universe afford Inflation?
108
A&S: How to calculate the inflationary fluctuation the
Darwinian cosmology with Λ :1) Use standard work on tunneling into inflation (“free lunch”, “universe in a garage”)
Farhi Guth & Gueven; Blau Gundelman & Guth; Fischler Morgan & Polchinski
2) Use stat mech to determine Pc for the classical solutions in 1)
inf c qP P P
quantum tunneling
Probability to form “incoming” classical solution
AA & Sorbo hep-th/0405270
II.5 Can the Universe afford Inflation?
109
Picture from A. Guth
qP
cP
II.5 Can the Universe afford Inflation?
110
• The stat mech piece for
de Sitter space with a small perturbation looks Schwarzschild far from the perturbation:
BHA A A A
Gibbons & Hawking
cP
II.5 Can the Universe afford Inflation?
111
• The stat mech piece for
de Sitter space with a small perturbation looks Schwarzschild far from the perturbation:
BHA A A A
Gibbons & Hawking
So
C BH I BHS S S S S S S S 4
infP
I dSI
mS S
m
where
cP
Dominated by reduction in entropy of full system (not SI)
II.5 Can the Universe afford Inflation?
112
• Box of gas analogy
Rare fluctuation in a box of gas:
(1 ),V f T
, 'gfV T
fV
f fraction of V affected
g size of fluctuation as a fraction of fV
Assuming entropy density (s) obeys3s T
1/ 41fluct eqm eqmS S f S fg
and using conservation of energy
Entropy of remaining “normal” region
Entropy of “weird” region
4E Vol T
fluct eqmS S
fluctP e
1/ 4(1 )eqm eqmS f g S fe e The dominant effect is that a volume fV has been deprived of eqm entropy
II.5 Can the Universe afford Inflation?
113
The Answer:
C BHS S S S
C
BH
SS S
C S
eP e
e
II.5 Can the Universe afford Inflation?
114
The Answer:
C BHS S S S
and
C
BH
SS S
C S
eP e
e
4P
I
m
mQP e
4
inf
PBH
I
mS S
mC QP P P e
II.5 Can the Universe afford Inflation?
115
The Answer:
C BHS S S S
and
C
BH
SS S
C S
eP e
e
4P
I
m
mQP e
4
inf
PBH
I BH
mS S
m S SC QP P P e e
Dominated by “entropy lost by environment”
II.5 Can the Universe afford Inflation?
116
Compare with “regular big bang”
8510BBS
fluct
BB
SS S
BB S
eP e
e
II.5 Can the Universe afford Inflation?
117
Compare with “regular big bang”
8510BBS
so
fluct
BB
SS S
BB S
eP e
e
inf 1BH BH
BB BB
SS S S
S S SBB
P e e
P e e
85 510 10BB BHS S Inflation highly favored
II.5 Can the Universe afford Inflation?
118
inf 1BH BH
BB BB
SS S S
S S SBB
P e e
P e e
8510BB BHS S Inflation highly favored
This is a quantification of the standard intuition:
• Inflation starts with a “cheap” fluctuation vs Standard Big Bang
• This makes a inflation “more likely” start for our observed universe.
II.5 Can the Universe afford Inflation?
119
BUT
120
Outside observer sees in-falling object take infinite time to reach the horizon (“never reaches the horizon”)
iii. Horizons, Entropy and Causal Patch Physics
Black Hole Event Horizon (schematic):
II.5 Can the Universe afford Inflation?
121
Outside observer sees in-falling object take infinite time to reach the horizon (“never reaches the horizon”)
Black Hole Event Horizon (schematic):
Principles of Causal Patch Physics:
• To the outside observer there is no “inside of Black Hole”
• Infalling observer reuses the same degrees of freedom to describe the interior* (outside observer absent)
• Could resolve BH info paradox
iii. Horizons, Entropy and Causal Patch Physics
*Requires highly non-local transformation between frames (“stringy magic”?)
II.5 Can the Universe afford Inflation?
122
Implications of causal patch physics for our calculations:
• Basis for De Sitter space as finite closed system & application of stat mech
• During inflation (quasi-De Sitter) a horizon forms: Possibly dramatic implications.
• Dyson Kleban & Susskind: There is no “outside the De Sitter horizon” during inflation. All degrees of freedom are inside.
II.5 Can the Universe afford Inflation?
123
• Principles of causal patch physics change everything:
DKS: A horizon forms for the inflating region and holographic magic is evoked:
de Sitter + small fluctuation (mass M)
( )dS BH MA A A
“Magic”
Inflation: approximate de Sitter
degrees of freedom re-organize to only describe inside the horizon.
Most degrees of freedom must “condense out” to manifest the very low inflationary entropy.
4
2inf
PI I I
I
mS A H S
m
II.5 Can the Universe afford Inflation?
124
• Principles of causal patch physics change everything:
DKS: A horizon forms for the inflating region and holographic magic is evoked:
de Sitter + small fluctuation (mass M)
( )dS BH MA A A
“Magic”
Inflation: approximate de Sitter
degrees of freedom re-organize to only describe inside the horizon.
Most degrees of freedom must “condense out” to manifest the very low inflationary entropy.
4
2inf
PI I I
I
mS A H S
m
BHS S Se
125
• Causal patch principles replace
inf 1BH
BB
SS
SBB
P e
P e
with
4
inf 1
P
II
BB BB
m
mS
S S S S S SBB
P e e
P e e
Inflation highly
disfavored
Inflation highly favored
II.5 Can the Universe afford Inflation?
126
• Causal patch principles replace
inf 1BH
BB
SS
SBB
P e
P e
Inflation highly favored
with
4
inf 1
P
II
BB BB
m
mS
S S S S S SBB
P e e
P e e
Low entropy of inflating region converted from benefit to liability
Inflation highly
disfavored
Counting of exterior makes inflation cheap
II.5 Can the Universe afford Inflation?
127
v. Discussion & Conclusions
Topics
• Transcending the specifics of de Sitter eqm
• Boltzmann’s Brain
• Conclusions
II.5 Can the Universe afford Inflation?
128
• Transcending the specifics of de Sitter eqm
This looks like a problem no matter how confused you are about what to put here
4
inf 1
P
II
BB BB
m
mS
S S S S S SBB
P e e
P e e
II.5 Can the Universe afford Inflation?
129
This is rare no matter how poorly you understand the entropy at Time 1
Time 1Time 2
II.5 Can the Universe afford Inflation?
130
And this is even more rare!
Time 1Time 2
II.5 Can the Universe afford Inflation?
131
1010S
Surely this is rare too
landscape
II.5 Can the Universe afford Inflation?
132
1010S
and this!
Eternal inflation
II.5 Can the Universe afford Inflation?
133
Landscapes and eternal inflation etc do not obviously get you off the hook.
For example for large spaces, consider the
limit
0
( )S
This looks like a
problem no matter how confused you are about what to put here
4
inf 1
P
II
BB BB
m
mS
S S S S S SBB
P e e
P e e
II.5 Can the Universe afford Inflation?
134
• Boltzmann’s Brain paradox:
The most likely fluctuation consistent with everything you know is your brain fluctuating out of chaos and immediately re-equilibrating. (Also works for planets) [Related to in DKS]
Only inflation has an answer to this paradox. With inflation, most probable way to create one brain (or planet) comes packaged with a huge flat universe (+body, fellow creatures etc)
This is as least as important as the other successes of inflation!
BB XBBP P
135
•Conclusions
Darwinian cosmology is better
DKS /AS/Λ offer an attractive scheme for Darwinian cosmology. Can bring discussions of inflation/etc to next level.
Cosmology appears to place causal patch physics in conflict with inflation (even when not using Λ eqm.).
Fundamental issue: Is there really more universe outside the horizon during inflation? (yes inflation OK)
Resolving this conflict between will teach us something very interesting about at least one of these:
-inflation
-causal patch physics
-quantum gravity
II.5 Can the Universe afford Inflation?
136
END
137
Burning question:
What is the most likely fluctuation to “give what we see:?:
-Normal Big Bang?
-Inflating Region?
138
Additional material
139
Where to go from here:
• How to fit all this into a “big picture”
- Can inflation be “eternal”? (Brode, Vilenkin, Guth, Aguirre & Gratton)
- Connection with quantum gravity, quantum measurement… (Banks, Banks & Fischler, Dyson et al, AA Kaloper & Song)
- Quantify “dominant channel” claim
- etc.
• Evaluate competing ideas:
- Ekpyrotic (no “attractor”, no volume factors. How can this channel compete?... a super-rare fluctuation)
- Cyclic (“a perpetual motion machine of the 2nd kind”?)
- Holographic (built in arrow of time)
II.4 Implications
140
More thoughts
Q: Can the thermodynamic arrow of time be sufficiently tightly linked with emergence of classicality to reduce waste of data as input?
(Do classical “regions” automatically have a “low S end”?)
Related to standard “wavefunction of the universe” work
II.4 Implications
Does gravity radically transform the nature of the arrow of time?
141
More thoughts:
-Sort our measures! (Usually we can handle this.)
- How can we contemplate the “general chaotic state of all possibilities”?
vs eternal inflation,
vs causal patch physics
II.4 Implications
142
Evaluate alternatives
• Attractor behavior vs “statement of state” (i.e ekpyrotic)
• Special initial conditions must be somewhere (vs. early statements about the “new” cyclic universe)
II.4 Implications
143
Idea“Creates” IC’s(attractor behavior)
Volume
Factors
Standard Big Bang no
Holographic Cosmology (Banks & Fischler)**
Inflation (Chaotic = ++)Wavefunction of Univ.
?
VSL Cosmology
Ekpyrotic Universe no
Eternal (Aguirre & Gratton)
New Cyclic
II.4 Implications
no
no
yes yes
yes (w/inflation)
yes “Yes”no
Version 1Version 2
no Xyes yes
no X
no
144III Conclusions
I) Inflation in the era of WMAP
I.1 Successes
I.2 Future tests
I.3 Theoretical advances
Exciting future
145
Why wonder about arrow of time inflation?
• Understand what we are really trying to accomplish with inflation a more solid foundation
Inflation:
1) Can not take all possible initial conditions into SBB
2) Can give “dominant channel” to Standard Big Bang.. (Still have predictive power, successful so far)
3) Solves the “Boltzmann’s Brain” problem
III Conclusions
II) Inflation and the arrow of time
-Initial attractor
-Volume factor
Special inflaton initial state (arrow of time) Required of all theories
146
Why wonder about arrow of time inflation?
• Evaluate “alternatives to inflation”
1) Attractor behavior is not the same as “statement of state”
2) Arrow of time all theories of initial conditions require something “special” (not completely generic)
3) (No Perpetual Motion!)
III Conclusions
II) Inflation and the arrow of time
“Statement of state” much less ambitious
147
Why wonder about arrow of time inflation?
III Conclusions
II) Inflation and the arrow of time
•Window on current hot topics
1) Singularities in quantum gravity
2) “Equilibrium” states in quantum gravity
3) Entropy and gravity (“Holography”) (AA, NK, Y-SS)
4) “Before” inflation
5) Arrow of time in quantum gravity
148
Why wonder about arrow of time inflation?
• Fun combination of physics ideas
III Conclusions
II) Inflation and the arrow of time