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Cosmic challenges for Cosmic challenges for fundamental physics fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe
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Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Dec 19, 2015

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Page 1: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Cosmic challenges forCosmic challenges forfundamental physicsfundamental physics

Diederik Roest December 9, 2009

Symposium “The Quantum Universe”

Page 2: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”
Page 3: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Modern cosmologyModern cosmology

Supernovae (SNe)

Cosmic Microwave Background (CMB)

Baryon AcousticOscillations (BAO)

What are the ingredients of the universe?

Page 4: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

SupernovaeSupernovae

Page 5: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Cosmic Microwave Cosmic Microwave BackgroundBackground

Page 6: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Baryon acoustic oscillationsBaryon acoustic oscillations

Page 7: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Putting it all Putting it all togethertogether

Page 8: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Concordance ModelConcordance Model

Nearly flat Universe, 13.7 billion years old.

Present ingredients: 73% dark energy 23% dark matter 4% SM baryons

Page 9: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

InflationInflation Period of accelerated

expansion in very early universe

CMB anisotropies confirm inflation as source of fluctuations

Inflationary properties are now being measured

Planck satellite:– Non-Gaussianities?– Tensor modes?– Constraints on inflation?

[cf. talk by Jan Pieter van der Schaar]

Page 10: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Cosmic challenges for fundamental

physics!

Cosmic accelerationCosmic acceleration

Two periods of accelerated expansion: inflation in very early universe present-time acceleration

No microscopic understanding.

Page 11: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Cosmic acceleration Cosmic acceleration

Modelled by scalar field with non-trivial scalar potential V

Can we get such potentials from string theory? Extreme case with extremum of scalar potential leads to De Sitter space-time.

Page 12: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

StringsStrings

Quantum gravity No point particles, but small

strings Unique theory Bonus: gauge forces

Unification of four forces of Nature?

Page 13: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

……and then some!and then some!

Super-symmetry

Dualities

Many vacua (~10500)?

Extradimensions

Branes& fluxes

String theory has many implications:

How can one extract 4D physics

from this?

Page 14: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

CompactificationsCompactifications

Page 15: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Stable compactificationsStable compactifications

Simple compactifications yield massless scalar fields, so-called moduli, in 4D.

Would give rise to a new type of force, in addition to gravity and gauge forces. Has not been observed!

Need to give mass terms to these scalar fields (moduli stabilisation).

Extra ingredients of string theory, such as branes and fluxes, are crucial!

energy

Scalar field

with fluxes and branes

simple comp.

Page 16: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Building a bridgeBuilding a bridge

What are the scalar potentials that follow from string theory, and do these allow for cosmologically interesting solutions?

Focus of my VIDI project “How stable are extra dimensions?” (2008-2013). Keywords: flux compactifications, moduli stabilisation.

Upcoming results: Relations between N=2, 4 and 8 supergravity models

with (un)stable dS vacua [1]? Higher-dimensional origin in terms of gauge, geometric

or non-geometric fluxes [2]?[1: D.R., Rosseel - in progress]

[2: D.R. ’09, Dibitetto, Linares, D.R. – in progress]

Page 17: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

ConclusionsConclusions

Modern cosmology requires accelerated expansion for dark energy and inflation

Can we use string theory to explain this? What are the scalar potentials from string

compactifications?(flux compactifications and moduli

stabilisation) Many interesteresting (future) results – both

theoretical and experimental

Page 18: Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”

Thanks for your attention!Thanks for your attention!

Diederik Roest December 9, 2009

Symposium “The Quantum Universe”