Transcript Document

String Inflation
@ Very Early Universe + 25
C.P. Burgess
with N. Barnaby, J.Blanco-Pillado, J.Cline, K. das Gupta,
C.Escoda, H. Firouzjahi, M.Gomez-Reino,
R.Kallosh, A.Linde,and F.Quevedo
Outline
• String inflation
• Why build models only a mother could love?
• Emerging features
• Mechanisms and naturalness issues
• Multiple scalars and robustness
• Mind-broadening: cosmic strings; reheating; …
• Open issues
• Scales; control of approximations; …
VEU + 25
Outline
• String inflation
• Why build models only a mother could love?
• Emerging features
• Mechanisms and naturalness issues
• Multiple scalars and robustness
• Mind-broadening: cosmic strings; reheating; …
• Open issues
• Scales; control of approximations; …
VEU + 25
Outline
• String inflation
• Why build models only a mother could love?
• Emerging features
• Mechanisms and naturalness issues
• Multiple scalars and robustness
• Mind-broadening: cosmic strings; reheating; …
• Open issues
• Scales; control of approximations; …
VEU + 25
String Inflation
• What might one
hope to learn?
• about strings
• about inflation
• Why is it hard?
VEU + 25
String Inflation
• What might one
hope to learn?
• about strings
• about inflation
• Why is it hard?
VEU + 25
String Inflation
• What might one
hope to learn?
• about strings
• about inflation
• Why is it hard?
Difficult to identify where we live within the string
landscape. Seek ‘modules’ encoding low-energy
features: standard model; dark energy; inflation; …
VEU + 25
String Inflation
• What might one
hope to learn?
• about strings
• about inflation
• Why is it hard?
VEU + 25
String Inflation
• What might one
hope to learn?
• about strings
• about inflation
• Why is
it hard?
Inflation
is under ever closer scrutiny due to the recent
wealth of cosmological data.
What are these measurements telling us?
VEU + 25
String Inflation
Batfit courtesy of Stephane Coutu
• What might one
hope to learn?
• about strings
• about inflation
• Why is
it hard?
Inflation
is under ever closer scrutiny due to the recent
wealth of cosmological data.
What are these measurements telling us?
VEU + 25
String Inflation
•
What we’d like string theory to tell us about inflation:
What might one
How generic is it in the landscape?
hope to learn?
Initial conditions, flat potentials, …
• about strings
• about inflation
• Why is it hard?
VEU + 25
String Inflation
•
What we’d like string theory to tell us about inflation:
What might one
How generic is it in the landscape?
hope to learn?
Initial conditions, flat potentials, …
• about strings
How does reheating work?
Does SM couple strongly enough to inflaton?
• about inflation
Do other channels couple even more strongly?
• Why is it hard?
VEU + 25
String Inflation
•
•
What we’d like string theory to tell us about inflation:
What might one
How generic is it in the landscape?
hope to learn?
Initial conditions, flat potentials, …
• about strings
How does reheating work?
Does SM couple strongly enough to inflaton?
• about inflation
Do other channels couple even more strongly?
How robust are inflationary inferences drawn
Why is it using
hard?
simple single-field slow-roll models?
VEU + 25
String Inflation
•
•
What we’d like string theory to tell us about inflation:
What might one
How generic is it in the landscape?
hope to learn?
Initial conditions, flat potentials, …
• about strings
How does reheating work?
Does SM couple strongly enough to inflaton?
• about inflation
Do other channels couple even more strongly?
How robust are inflationary inferences drawn
Why is it using
hard?
simple single-field slow-roll models?
Are qualitatively new kinds of signatures or
mechanisms possible?
VEU + 25
Emerging Picture
• Mechanisms
• Robustness
• Mind broadening
VEU + 25
Emerging Picture
• Mechanisms
• Robustness
• Mind broadening
VEU + 25
Emerging Picture
• Mechanisms
• Robustness
Why is it so hard to find inflation in string theory?
• Mind broadening
It has many scalars, which SUSY gives flat potentials,
but SUSY breaking is hard to compute reliably.
VEU + 25
Emerging Picture
• Mechanisms
• Robustness
What is so hard about finding inflation in string theory?
• Mind broadening
It has many scalars, which SUSY gives flat potentials,
but SUSY breaking was hard to compute reliably.
A convincing case for inflation requires knowing the
potential for all of the relevant low-energy fields.
VEU + 25
Emerging Picture
Giddings, Kachru & Polchinski
Kachru, Kallosh, Linde & Trivedi
•
For Type IIB strings it is now known how to compute
Mechanisms
the potentials for many of these scalars, when close to
an N=1 4D vacuum.
• Robustness
Key ingredients:
•
D3 and D7 branes &
orientifolds
Mind Fluxes
broadening
sourced by these
branes, wrapping extra
dimensions
Gmnp  H mnp   Fmnp
VEU + 25
Emerging Picture
Klebanov & Strassler
• Mechanisms

ds 2  h 1/ 2mndx mdx n  h1/ 2 dr 2  r 2d2
h  1/ r4
dr 2
ds  r mndx dx  2  d2
r
2
• Robustness

2
m
n
Strongly warped throats
arise in response to specific
flux configurations.
• Mind broadening
Warped throats strongly
redshift energies à la
Randall & Sundrum
VEU + 25
Emerging Picture
Denef & Douglas
• Mechanisms
• Robustness
•
K  2 ln V  2 ln 13 / 2   23 / 2 
W  W0  A1ea1T1  A2ea2T2
f i ab  Ti  ab
Low-energy dynamics of
last few moduli are
by a low-energy
Mind described
broadening
4D supergravity.
Inflationary solutions make
sense if H ¿ MKK
VEU + 25
Emerging Picture
BMNQRZ
Dvali et al
KKLMMT
Silverstein & Tong
Baumann et al
Two classes of moduli to be considered as inflatons
• Mechanisms
Brane-antibrane separation
• Robustness
• Mind broadening
VEU + 25
Emerging Picture
CB, Quevedo, Rajesh & Zhang
Blanco-Pillado et al
Conlon & Quevedo
Bond, Kofman & Prokushkin
Two classes of moduli to be considered as inflatons
• Mechanisms
•
Rolling moduli
(volume and shape of extra
Robustness
dimensions, or their
superpartner axions)
• Mind eg:
broadening
Better Racetrack:
K  2 ln V  2 ln 13 / 2   23 / 2 
W  W0  A1ea1T1  A2ea2T2
f i ab  Ti  ab
VEU + 25
Emerging Picture
• Mechanisms
• Robustness
• Mind broadening
VEU + 25
Emerging Picture
•
In all cases the inflationary dynamics involves multiple
Mechanisms
fields moving in a complicated potential. Slow rolls
appear not to be generic.
• Robustness
•
Warning: It is insufficient
in all known cases to fix
fields by hand, while
Mind some
broadening
evolving others (despite
there being many papers
which do so).
VEU + 25
Emerging Picture
Blanco-Pillado et al
•
Single-field slow-roll analyses nonetheless capture much
Mechanisms
of the generic predictions for the CMB
• Robustness
But must check: The
•
presence of multiple
scalars allows in
new features
Mind principle
broadening
like isocurvature
perturbations, etc.
VEU + 25
Emerging Picture
•
Because inflation is found in 4D effective theory,
Mechanisms
predictions tend to be contained within those of the
corresponding 4D mechanism
• Robustness
Small-field models
•
Large-field models
models
Mind Hybrid
broadening
VEU + 25
Emerging Picture
Kallosh & Linde
Baumann & McAllister
•
Because inflation is found in 4D effective theory,
Mechanisms
predictions tend to be contained within those of the
corresponding 4D mechanism
• Robustness
Small-field models
•
Large-field models
models
Mind Hybrid
broadening
Only stringy
implication so far is
small tensor amplitude
VEU + 25
Emerging Picture
Kaloper, Kleban, Lawrence & Shenker
CB, Cline, Holman & Lemieux
•
Heavy physics (M À H) decouples in string theory, and
Mechanisms
so tends not to interfere with inflationary predictions.
• Robustness
Two kinds of effects can
•
be larger than the naïve
H2/M2 suppression:
Mind Non-adiabatic
broadeningeffects
near horizon exit;
or
m2/M2 where H = m2/Mp
H-1(t)
Length
10-30 e-foldings
Inflation
(t)
Post-Inflation
oscillations
60 e-foldings
p
Time
VEU + 25
Emerging Picture
Conlon & Quevedo
•
Inflation may be more natural in Kahler modulus
Mechanisms
inflation, with 3 moduli in large-volume framework.
• Robustness

K  2 ln  13 / 2   23 / 2   33 / 2   

W  W0  A1ea1T1  A2ea2T2  A3ea3T3
f i ab  Ti  ab
• Mind Slow
broadening
roll relies on large field values rather than tuned
parameters in the potential
Veff  A  B( / M )n exp  b( / M )n


 i  ( / M )n À 1
VEU + 25
Emerging Picture
• Mechanisms
• Robustness
• Mind broadening
VEU + 25
Emerging Picture
BMNQRZ
Dvali et al
Several novel features and mechanisms have emerged
• Mechanisms
Brane-antibrane annihilation, and the absence of the
inflaton in the post-inflationary low-energy theory;
• Robustness
• Mind broadening
VEU + 25
Emerging Picture
Barnaby et al
Kofman & Yi
Chialva, Shiu & Underwood
Langfelder
Several novel features and mechanisms have emerged
• Mechanisms
Brane-antibrane annihilation, and the absence of the
inflaton in the post-inflationary low-energy theory;
• Robustness
Warped reheating, and the relatively efficient cascade
of inflationary energy into the lowest throat.
• Mind broadening
VEU + 25
Emerging Picture
Sarangi & Tye
BMNQRZ
Jones, Stoica & Tye
Copeland, Myers & Polchinski
Several novel features and mechanisms have emerged
• Mechanisms
Brane-antibrane annihilation, and the absence of the
inflaton in the post-inflationary low-energy theory;
• Robustness
Warped reheating, and the relatively efficient cascade
of inflationary energy into the lowest throat.
• Mind broadening
Cosmic strings, and the leaving of inflationary relics.
VEU + 25
Emerging Picture
Silverstein & Tong
Several novel features and mechanisms have emerged
• Mechanisms
Brane-antibrane annihilation, and the absence of the
inflaton in the post-inflationary low-energy theory;
• Robustness
Warped reheating, and the relatively efficient cascade
of inflationary energy into the lowest throat.
• Mind broadening
Cosmic strings, and the leaving of inflationary relics.
Inflation from relativistic motion (DBI inflation)
VEU + 25
Emerging Picture
Khoury, Ovrut, Steinhardt & Turok
Other ways our minds may yet broaden:
• Mechanisms
Are there stringy alternatives to inflation?
• Robustness
• Mind broadening
VEU + 25
Open Issues
• Problem of scales
• Control over
approximations
VEU + 25
Open Issues
• Problem of scales
• Control over
approximations
VEU + 25
Open Issues
Kallosh & Linde
CB, Quevedo, Rajesh & Zhang
•
•
To address reheating issues must know where ‘we’ live
Problem
and of
howscales
we couple to the inflating sector.
Problem: in the available models the string scale, Ms,
required to obtain the right amplitude for primordial
scalar
perturbations gives a supersymmetry breaking
Control
over
scale which is too high to solve the hierarchy problem.
approximations
eg: for warped models: cannot make 2nd throat too
deep if inflation occurs in 1st throat
or: for large-volume models:
Ms ~ Mp/V1/2; m3/2 ~ Mp/V ~ Ms/V1/2
VEU + 25
Open Issues
Possible ways out:
• Problem of scales
Low-scale inflation (German, Ross & Sarkar)
•
Generate inflationary perturbations through other
Control
over
means
(eg: a curvaton mechanism – nongaussianity?)
approximations
Allow Ms to roll to larger values after inflation
(Conlon, Kallosh, Linde & Quevedo)
VEU + 25
Open Issues
• Problem of scales
• Control over
approximations
VEU + 25
Open Issues
•
•
String inflation models are baroque in order to keep
Problem
of scales
control
over all approximations being used.
Some remaining weaknesses:
Size of corrections to the equations used
Control* over
if dynamics is not given as a 4D supergravity
approximations
* if SUSY breaking comes from anti-branes
VEU + 25
Open Issues
•
•
String inflation models are baroque in order to keep
Problem
of scales
control
over all approximations being used.
Some remaining weaknesses:
Size of corrections to the equations used
Control* over
if dynamics is not given as a 4D supergravity
approximations
* if SUSY breaking comes from anti-branes
Inflation seekers scan through parameters of 4D action
as if these are free and not calculable.
VEU + 25
Outlook
• There are plausible formulations of inflation in string
theory, but still at the stage of mapping out what is
possible
• Not easy to obtain and keep control over approximations
VEU + 25
Outlook
• There are plausible formulations of inflation in string
theory, but still at the stage of mapping out what is
possible
• Not easy to obtain and keep control over approximations
• Possible progress on fine-tunings, but not generically
VEU + 25
Outlook
• There are plausible formulations of inflation in string
theory, but still at the stage of mapping out what is
possible
• Not easy to obtain and keep control over approximations
• Possible progress on fine-tunings, but not generically
• New insights on reheating (warping, cosmic strings);
VEU + 25
Outlook
• There are plausible formulations of inflation in string
theory, but still at the stage of mapping out what is
possible
•
•
•
•
Not easy to obtain and keep control over approximations
Possible progress on fine-tunings, but not generically
New insights on reheating (warping, cosmic strings);
Inflationary signals largely robust, except near horizon exit
VEU + 25
Outlook
• There are plausible formulations of inflation in string
theory, but still at the stage of mapping out what is
possible
•
•
•
•
•
Not easy to obtain and keep control over approximations
Possible progress on fine-tunings, but not generically
New insights on reheating (warping, cosmic strings);
Inflationary signals largely robust, except near horizon exit
Small tensor perturbations?
VEU + 25
Outlook
• There are plausible formulations of inflation in string
theory, but still at the stage of mapping out what is
possible
•
•
•
•
•
Not easy to obtain and keep control over approximations
Possible progress on fine-tunings, but not generically
New insights on reheating (warping, cosmic strings);
Inflationary signals largely robust, except near horizon exit
Small tensor perturbations?
• Possibly even more novel physics can arise!
VEU + 25
Outlook
• There are plausible formulations of inflation in string
theory, but still at the stage of mapping out what is
possible
•
•
•
•
•
Not easy to obtain and keep control over approximations
Possible progress on fine-tunings, but not generically
New insights on reheating (warping, cosmic strings);
Inflationary signals largely robust, except near horizon exit
Small tensor perturbations?
• Possibly even more novel physics can arise!
VEU + 25
fin
VEU + 25