The%20LARGE%20Volume%20Scenario:%20Realisation%20and%20Cosmological%20Implications - PowerPoint PPT Presentation

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The%20LARGE%20Volume%20Scenario:%20Realisation%20and%20Cosmological%20Implications

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(Explicit form of K, W, f. For N=1 compactifications) Why LARGE volume? ... Simplest case ?=1/3. General Conditions for LARGE Volume. h12 h11 1 ... – PowerPoint PPT presentation

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Title: The%20LARGE%20Volume%20Scenario:%20Realisation%20and%20Cosmological%20Implications


1
The LARGE Volume Scenario Realisation and
Cosmological Implications
F. Quevedo, Cambridge. Liverpool, March 2008.
  • M. Cicoli, J. Conlon, FQ, 0708.1873 hep-th
    to appear
  • J. Conlon, R. Kallosh, A. Linde, FQ, to appear

Related talks E. Plauschinn and E. Palti
2
String Phenomenology
  • Explicit Realistic Models
  • (SU(3)xSU(2)xU(1), 3 families, etc.)
  • Model Independent Issues
  • (axions, no-global symmetries,.,SUSY breaking,
    moduli stabilisation,)
  • 4D Effective Actions
  • (Explicit form of K, W, f. For N1
    compactifications)

3
Why LARGE volume?
  • Effective field theory robust
  • Phenomenology M2PlanckM2string V

V104 MstringMGUT1017GeV V1030
Mstring1 TeV V1015 Mstring1011 GeV (Also
RS warping !)
4
MODULI STABILISATION?
5
Exponentially Large Volumes in IIB
6
Perturbative vs Non perturbative
  • In general
  • Then
  • Usually V0 dominates but V00 (no-scale
    )
  • Dominant term is VJ unless W0ltlt1 (KKLT)

7
Exponentially Large Volumes
BBCQ, CQS (2005)
  • Perturbative (alpha) corrections to K
  • At least two Kähler moduli (h21gth11gt1)

Example
8
as2p/gs N
Exponentially large volumen !!!
String scale Ms2M2Planck/V W01-10 Ms1 TeV
problematic from 5th force
9
Universe D3 Brane or D7 Brane
10
Standard Model on D7 Branes
  • Solve hierarchy problem Mstring 1011 GeV!
  • W01 (no fine tuning)
  • Kahler potential for chiral matter computed


Conlon, Cremades, FQ (2006)
11
The Standard Model in the CY
12
Chiral Matter on D7 Branes Soft SUSY Breaking
terms
Conlon et al.
  • Universality!
  • No extra CP violation!
  • Mi m3/2 / log (Mp/m3/2)
  • String scale 1011 GeV
  • Solves hierarchy problem!

Simplest case ?1/3
13
General Conditions for LARGE Volume
  • h12 gt h11 gt 1
  • At least one blow-up mode (point-like
    singularity)
  • Blow-up mode fixed by non-perturbative effects,
    volume by alpha corrections
  • For Nsmall blow-up modes, there are
    Lh11-Nsmall-1 flat directions at tree-level
  • These directions are usually lifted by
    perturbative effects
  • L moduli lighter than
    volume!

14
String Loop Corrections
Berg-Haack-Kors Berg-Haack-Pajer
Leading order correction for V is alpha but
string loops relevant to fix other moduli
15
Example 1
Blumenhagen et al
TauSM
16
Example 2 K3 Fibrations
  • K3 Fibration with 2 Kahler moduli 1,1,2,2,6
    model
  • No LARGE volume

17
  • K3 Fibration with 3 Kahler moduli (one blow- up)
  • tau3 small, tau 1 and tau 2 LARGE

18
V
W
W
Volume, W
19
COSMOLOGY
  • (Inflation, Cosmological moduli problem, etc.)

20
BRANE - ANTIBRANE INFLATION
All branes inflate while two approach Inflaton
Open string mode (talks by R. Gregory, M. Haack
and H. Stoica)
21
KAHLER MODULI INFLATION
  • Candidate Inflatons Closed string modes
  • Kahler Moduli (size/axion)
  • Small modulus inflaton

22
Kähler Moduli Inflation
Conlon-FQ Bond-Kofman-Prokushkin
Calabi-Yau h21gth11gt2
Small field inflation No fine-tuning!! 0.960ltnlt0.9
67
V
tn
volume
23
Open Questions
  • Loop effects tend to spoil flatness
  • Non tensor perturbations (rT/Sltltlt1)?
  • Tension phenomenology vs cosmology

Gravitino mass 1 TeV/Gravitino mass gtgt 1 TeV
?? (string scale 10 11 GeV/ string scale GUT
scale)
24
Low Energy SUSY vs Inflation
  • Low scale inflation?
  • Runaway before reheating?

Ross et al,
Conlon, Kallosh, Linde, FQ
25
No Overshooting problem!!!
26
New Candidate Inflatons
  • Lh11-Nsmall-1 almost flat directions are light
  • MassV-5/3lt Volume modulus mass
  • mV-3/2H
  • Recall ? mass2/H

Cicoli et al.
27
After Inflation
28
Physics of Moduli Fields
  • Dilaton and Complex Structure
  • Small (heavy) Kahler moduli
  • Large (light) Kahler modulus

Moduli masses
Volume axion mexp(-V)ltlt10-33 eV (equality if
MstringMGUT)!
29
Summary of couplings
30
Other Cosmological Implications
J.Conlon, FQ
  • Cosmological moduli problem
  • Observational implications of light volume
    modulus?

DCQR, BKN
U,S trapped at their minimum T except for
volume, heavy and decay fast ! (No CMP nor
gravitino overproduction) Volume (mass MeV) CMP
Gamma rays, e-e-
31
The 511 keV Line
32
INTEGRAL/ SPI 511 keV line
Light Modulus ? Dark matter? Mass 1MeV,
coupling to electrons dominant 511 keV from
volume modulus decay? (prediction!) BUT almost
ruled out 2 months ago!!!
33
Intensity
INTEGRAL
34
General Picture
  • Nsmall heavy Kahler moduli (cosmological
    harmless)
  • Volume modulus (CMP 511 keV line predicted
    monochromatic line!) (see Boyarski et al)
  • Lh11-Nsmall-1 lighter moduli (candidate
    inflatons, CMP, new monochromatic lines!!
    (observable?))
  • CMP (late low energy inflation?)

35
Conclusions
  • Non-perturbative effects fix only a fraction of
    Kahler moduli (Nsmall)
  • Alpha effects fix volume to exponentially large
    values (Both LARGE volume and large warping in
    the same class of models!?)
  • Loop corrections needed to fix the rest of Kahler
    moduli
  • Interesting phenomenology/cosmology
  • Astrophysics (forest of monochromatic lines?)
  • Fully realistic model?

36
Solution of CMP?Thermal Inflation
LythStewart (1995)
Number of e-folds
N10 dilutes moduli
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