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Title: Flux Compactifications Accelerating Universes And All That


1
Flux Compactifications Accelerating Universes
And All That
  • Sandip Trivedi
  • Tata Institute of Fundamental Research, Mumbai,
    India
  • Goa Jan. 07

2
  • Introduction Motivation
  • Type IIB Strings with Fluxes
  • Supersymmetry Breaking and de Sitter Universe.
  • The Landscape and Conclusions

3
Some References
  • Flux Compactifications
  • Giddings Kachru, Polchinski, hep-th/0105097
  • Douglas and Kachru, hep-th/0610102
  • Kachru, Kallosh, Linde, S.P.T., hep-th/0301240

4
Some References
  • The Landscape
  • Bousso and Polchinski, hepth/0004134
  • Susskind hep-th/0302219
  • Susskind The Cosmic Landscape

5
Introduction
  • Flux Compactifications
  • String Theory Requires 10 dimensions.
  • Extra 6 dimensions are small. curled up.
  • Many Possibilities, e.g. Calabi Yau manifolds.
  • Any particular Calabi Yau manifold can take many
    different sizes and shapes.

6
Introduction
  • These are examples of Moduli
  • O(100) Moduli is common.
  • In a Field Theory description these are Flat
    directions.

7
Moduli Stabilisation
  • Typically Many Flat Directions in String
    Compactifications. (100)
  • Different Sizes and Shapes.


Physical Parameters e.g., G_N, alpha, vary along
these directions
8
Moduli and their Problems
  • These flat directions are a problem.
  • Typically they will be lifted once supersymmetry
    is broken.
  • Cosmology
  • However if mass is small they will overclose the
    universe (Mgt10 Tev)

9
String Theory Typically lead to run-away
situations. Not stable vacua.
10
Flux Compactifications
Main Advantage Flux gives rise to controlled
ways of stabilising the Moduli and Breaking
Supersymmetry.
11
Flux Compactifications
  • Important In Phenomenology
  • Calculate Standard Model Couplings
  • b) Supersymmetry Breaking

12
  • Important In Cosmology

Positive Vacuum Energy DeSitter Universe
Slowly Varying Potential Inflation
13
Flux Compactifications
  • Another Advantage
  • Concentrated Flux gives rise to large Warping.
  • Natural way to constructed models of Randall
    Sundrum (or large extra dimension) type.

14
6 Dim Calabi- Yau
Warped region with throat
Brane or String weighs less inside due to
gravitational red-shift
Warp Factor
15
Flux Compactifications
  • Curl Up Extra Dimensions while turning on Flux in
    these directions.
  • Flux generalisation of magnetic flux (including
    higher forms F_2,F_3,F_4, )
  • Gives extra potential energy depending on size
    and shape of compactification


16

Internal directions
Non-compact directions
17
FLUX COMPACTIFICATION
Why Does Flux Help?
Any Value of R1,R2 Allowed Moduli
R2
R1
Torus Is Flat, Curvature Vanishes.
18
Flux Compactifications
Size Modulus Shape Modulus
19
Turn On Magnetic Field
R2
AR1 R2
R1
Dirac Quantisation
Extra Cost In Energy
E
A
20
Type IIB String Theory Promising Corner to
Begin Giddings, Kachru, Polchinski Fluxes
Three-Forms Five-Form Branes D3
(fill 31 dimensions), D7, 03,07. (N0
5-Branes/Planes)
21
  • Type IIB String Theory
  • must be closed.
  • Such closed and non-trivial fluxes lie in a
    vector space. Its dimensionality is a
    topological invariant, .
  • Fluxes are also quantised.

22
Fluxes
Total Number of allowed Fluxes Exponential in
is finite, determined by tadpole condition

23
Fluxes
  • For reasonably big the total number of
    allowed fluxes can be very large.
  • is quite common.
  • This gives rise to an exponentially large number
    of vacua.

24
  • Type IIB String Theory
  • Take String Coupling to be small,
  • Work in Supergravity approximation. To be valid,
    the curvature should be small compared to .
    Also volume should be big compared to .

25
Basic Strategy
  • We will assume these approximations are valid and
    self-consistently find vacua where the required
    conditions are met.

26
Basic Strategy
  • Two Steps
  • First find Susy preserving vacua with all moduli
    stabilised.
  • Next break supersymmetry and find
  • (metastable) vacua.

27
I)
II)
28
  • I) Moduli Stabilisation With Susy
  • Internal Space E.g. Calabi Yau with
    identifications (Orientifold 3 and 7 planes).
  • Flux gives rise to a relatively minor
    modification of the internal space a warp
    factor.

29
More on Moduli Stabilisation
  • The moduli of interest are size and shape
    deformations of the Calabi-Yau space.
  • These get a mass, ,
  • where, , is the Radius of
    compactification.
  • Thus the lifting of these moduli can be studied
    in a 4 dim. Effective field theory.

30
Shape Moduli Stabilisation
  • A superpotential arises at tree-level.
  • This depends on the shape moduli and the
    axion-dilaton.
  • Generically this fixes all these moduli.

31
Shape Moduli Stabilisation
And is the holomorphic-three form on the
Calabi Yau, which depends on the shape moduli.
Gukov, Vafa, Witten Giddings, Kachru, Polchinski
32
Spectrum
String Modes
KK Modes
1/R
Shape Moduli
Size Moduli
33
Size Moduli Stabilisation
  • Non-perturbative Corrections to Superpotential
    can also arise.
  • These are dependent on Size moduli and can
    stabilise them.

34
Size Moduli Stabilisation
  • Two possibilities
  • Euclidean D3 Branes wrapping four-cycles of
    appropriate topology (ED3 action depends on size
    of cycle)
  • b) Non-perturbative gauge dynamics on coincident
    D7 branes

35
Size Modulus Stabilisation
  • Euclidean D3 Branes must wrap divisor whose
    Arithmetic genus is unity.
    Witten.
  • For D7-Branes wrapping divisors this condition
    need not be met. The Fluxes can lift additional
    zero modes.
  • Goerlich, Kachru, Tripathy, Trivedi

36
Example One Size Modulus
Shape moduli get a treel level mass and are
heavier. After Integrating them out resulting
effective theory for the size modulus is
37

38
For small we can get a large
39
if W_0 ltlt1. With 10(100) vacua this leaves many
possibilities.
40
Spectrum
String Modes
KK Modes
1/R
Shape Moduli
Size Modulus
41
  • II) Supersymmetry Breaking
  • Add anti-D3 brane
  • Warped geometry allows scale of susy breaking to
    be small

42
6 Dim Calabi- Yau
AdS_5 like region Which terminates
Anti D3 Brane at Bottom
Turn on Flux along a cycle of small size. This
concentrates the flux and gives rise to
significant warping.
43
Klebanov Strassler
6 Dim Calabi- Yau
AdS_5 like region Which terminates
Anti D3 Brane at Bottom
Warp factor at the Bottom
44
Supersymmetry Breaking and Uplifting
The anti D3 brane leads to an extra term

45
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46
  • Thus we see that all moduli are finally
    stabilised and supersymmetry broken.
  • And this allows us to obtain desitter vacua in
    string theory.

47
More on deSitter Vacua
Prior to this construction there were some No-go
Theorems which said that deSitter Universes could
not be arise. The obstruction was really that
moduli had not been stabilised and supersymmetry
was being broken, leading to run-away behaviour
and not deSitter vacua.
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49
Spectrum
String Modes
KK Modes
Shape Moduli
Size Modulus
gravitinio
50
  • By varying the relative strength of the anti-D3
    brane contribution and we can get
    either a negative or positive cosmological
    constant.
  • To get a small cosmological constant these would
    have to very precisely cancel. One would pay a
    price, but since there are many-many vacua to
    begin with this is still possible.

51
Ashok, Douglas
The number distribution of vacua for a small
cosmological constant is flat

52
The deSitter vacua are metastable. They can decay
by Coleman-Deluccia instantons or Hawking-Moss
instantons. Resultant lifetime
Easily bigger than years Smaller
than Poincare recurrence time
53
Bousso, Polchinski Susskind
Landscape
Many different vacua. Many different directions
Varying cosmological constants. Transitions
between them are possible.
54
Landscape
  • Many Questions
  • Is String Theory Predictive?
  • Who ordered all the other vacua?
  • How do we find the Standard Model vacuum?
  • Should we give up on Naturalness?
  • The Anthropic Principle?

55
Landscape
  • My Views
  • Anthropics Should be the last resort.
    Conventional explanations have testable
    consequences.

56
Landscape
  • Too early to conclude that string theory not
    predictive. By inputing some data(
    ) we might be able to predict a lot.
  • Key Question In coupling constant space how
    closely spaced are the standard model-like vacua.
    We dont know enough about the theory to answer
    this yet.
  • Also, understanding time, the initial singularity
    etc might help.

57
Landscape
  • What is clear though is that at our present
    level of understanding, String Theory is more
    akin to a general framework than a specific UV
    completion of the standard model.
  • So we should use it as a framework for model
    building and for understanding gauge theories.
  • This might well be its best use as we lead up to
    the LHC.

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Conclusions
Fluxes can help stablise all moduli. Resulting
Compactifications interesting for
phenomenology. And for Cosmology. Landscape here
to say.
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