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Moduli Stabilization:Moduli Stabilization:
A Revolution in String A Revolution in String Phenomenology / Cosmology ? Phenomenology / Cosmology ?
F. Quevedo SUSY 2005
The ProblemThe Problem
String/M-Theory unique but has many solutions String/M-Theory unique but has many solutions or vacua.or vacua.
Some solutions resemble the Standard Model Some solutions resemble the Standard Model and MSSM.and MSSM.
Degeneracy : Discrete + Continuous (SUSY) .Degeneracy : Discrete + Continuous (SUSY) .
Outstanding Problems:Outstanding Problems: SUSY breaking + Vacuum degeneracy.SUSY breaking + Vacuum degeneracy.
HistoryHistory
t<1986 Calabi-Yau String Compactifications: Many free t<1986 Calabi-Yau String Compactifications: Many free
moduli (size and shape of extra dimensions)moduli (size and shape of extra dimensions)
1986<t<1991 Gaugino condensation and T-1986<t<1991 Gaugino condensation and T-duality duality
1991<t<2002 More moduli! (D-brane positions)1991<t<2002 More moduli! (D-brane positions)
t>2002 GKP/ KKLT : Fluxes fix modulit>2002 GKP/ KKLT : Fluxes fix moduli
Dilaton S, Kähler TComplex structure U
Fix S and one T
CHSWCHSW
DIN, DRSW, K, FILQ, FMTVDIN, DRSW, K, FILQ, FMTV
……GKP, KKLT, …GKP, KKLT, …
KKLT ScenarioKKLT Scenario
Type IIB String on Calabi-Yau orientifoldType IIB String on Calabi-Yau orientifold
Turn on FluxesTurn on Fluxes ∫∫aa FF33 = n = n aa ∫ ∫bb HH33 = m = m bb
SuperpotentialSuperpotential W =W = ∫ ∫ GG33 ΛΛ ΩΩ, G, G3 3 = = FF3 3 –iS–iS HH33
Scalar Potential:Scalar Potential: V= e V= eKK |D |DaaW|W|22 MinimumMinimum D DaaW = 0 W = 0 Fixes UFixes Uaa and S and S T moduli unfixed: T moduli unfixed: No-Scale modelsNo-Scale models
Size of cycle a = USize of cycle a = Uaa
GKPGKP
To fix KTo fix Kähler moduli: Non-perturbative D7 effectsähler moduli: Non-perturbative D7 effects
FluxesFluxes Non-perturbativeNon-perturbative
VolumeVolume
SUSY AdS minimumSUSY AdS minimum
(W(W00 << 1) << 1)
Lifting to de Sitter (add anti D3 branes, D-terms, etc.)Lifting to de Sitter (add anti D3 branes, D-terms, etc.)
SUSY breaking termSUSY breaking term
KKLT, BKQ, SSKKLT, BKQ, SS
VV
axionaxion volumevolume
The LandscapeThe Landscape
Huge number of discrete Huge number of discrete vacua >10vacua >10500500
StatisticsStatistics
Randall-Sundrum Randall-Sundrum warping from strings!warping from strings!
Non SUSY de SitterNon SUSY de Sitter
Dark energy?Dark energy?
`SM’ on D3/D7branes`SM’ on D3/D7branes
Soft SUSY breaking?Soft SUSY breaking?
Inflation?Inflation?
AD, DD, DDF, GKTT,CQ,BGHLWAD, DD, DDF, GKTT,CQ,BGHLW
GKPGKP
BPBP
CG-MQUCG-MQU
Exponentially Large VolumesExponentially Large Volumes
At least two KAt least two Kähler moduli (hähler moduli (h2121>h>h1111>1)>1)
Perturbative corrections to KPerturbative corrections to K
Example :Example :
Exponentially large !Exponentially large !
BBCQ, CQSBBCQ, CQS
KKLT AdSKKLT AdS
Non SUSY AdSNon SUSY AdS
WW00~10~10-10-10
WW00<10<10-11-11
Both minima Both minima mergemerge
Soft SUSY BreakingSoft SUSY Breaking
From KKLT not explicit model but interesting general From KKLT not explicit model but interesting general behaviour (D/F term breaking, AMSB, …)behaviour (D/F term breaking, AMSB, …)
From lifting of large volume modelsFrom lifting of large volume models
MsMs~10~101313 GeV Gaugino masses ~ 10 GeV Gaugino masses ~ 1022 GeV, scalars m ~ GeV, scalars m ~ 101077 GeV GeV
Ms=MMs=MGUTGUT viable if warping, viable if warping,
Ms=Tev `viable’ if SM anti D-brane (but 5Ms=Tev `viable’ if SM anti D-brane (but 5thth force and cmp?) force and cmp?)
CFNOP,CJOCFNOP,CJO
CQSCQS
Matter on D3Matter on D3
INFLATION INFLATION
Racetrack InflationRacetrack Inflation
Topological eternal inflation !Topological eternal inflation !
Slow roll if 1/1000 fine tuning, Slow roll if 1/1000 fine tuning,
NN~60, ~60, δδHH~10~10-5 -5 for Ms~10for Ms~1015 15 GeVGeV
nnss ~ 0.95~ 0.95
B-PBCEG-RKLQB-PBCEG-RKLQ
D3 BraneD3 Brane
φφ
φφ inflaton field inflaton field
Brane- Antibrane inflationBrane- Antibrane inflation BMNRQZ, DSSBMNRQZ, DSS
KKLMMT, HKP, KTW, KKLMMT, HKP, KTW, FT, BCSQFT, BCSQ
Slow-roll (large field) inflation possible.Slow-roll (large field) inflation possible.
Need 1/1000 fine tuning of parameters to Need 1/1000 fine tuning of parameters to
get 60-efoldings (get 60-efoldings (ηη-problem)-problem)
NN~60, ~60, δδHH~10~10-5-5 for for
Ms~ 10Ms~ 101515 GeV GeV
nnss~1.05~1.05 BCSQBCSQ
VV
YYtachyontachyon
Tachyon complex topological defects Tachyon complex topological defects D (p-2) branes cosmic strings !D (p-2) branes cosmic strings !
End of inflation: Open string tachyonEnd of inflation: Open string tachyonBMNQRZBMNQRZ
ST, JST, CMPST, JST, CMP
S, BMNQRZS, BMNQRZ
Warped tachyonic inflationWarped tachyonic inflation
A,B depend on warping (fluxes) and E&M fields on non-A,B depend on warping (fluxes) and E&M fields on non-BPS brane. If A,BBPS brane. If A,B~1 no slow-roll~1 no slow-roll
AB large slow-rollAB large slow-roll
No fine-tuning! But need large fluxesNo fine-tuning! But need large fluxes
R, CQSR, CQS
INITIAL CONDITIONSINITIAL CONDITIONS
Sen’s open string Sen’s open string completeness completeness conjectureconjecture
t -tt -t
Pre big-bang ! ?Pre big-bang ! ?
Inflation and compactification or big-crunch/bangInflation and compactification or big-crunch/bang
and decompactification ! ?and decompactification ! ?
CONCLUSIONSCONCLUSIONS
Exciting timesExciting timesRS warping from CS sector, ADD large extra RS warping from CS sector, ADD large extra dimensions from Kdimensions from Kähler moduli sector.ähler moduli sector.Soft terms calculable for first time rich Soft terms calculable for first time rich phenomenologyphenomenologyExtensions to other string theoriesExtensions to other string theoriesConcrete models of inflationConcrete models of inflationSimple principles, complicated solutions, but SM Simple principles, complicated solutions, but SM is also ugly!is also ugly!Many open questionsMany open questions(A fully realistic model?)(A fully realistic model?)