Cosmology
Where are we ? Cosmology
CMB CMB P.Natoli 2009 Planck
Intensive robustness tests (M.Lejeune) Available on line : Impressive power for Cosmology
BASE CDM MODEL (Planck + lensing+WP + HL) PLANCK promised us precision cosmology… (1993)
ParameterValue (68%) bh2bh ± ch2ch ± * (acoustic scale at recombination) ± (~ 500 parts per million accuracy) 0.090±0.014 (WMAP “seeded”) ln(10 10 A s )3.087±0.024 nsns ± ( 5 ) H0H0 67.9±1.0 0.693±0.013 8 ±0.097 z re 11.1±1.1 BASE CDM MODEL (Planck + lensing+WP + HL) P.Natoli
Intensive robustness tests (M.Lejeune) Available on line : Impressive power for Cosmology (remember cosmology in 1993…)
More than primary Cl… More than primary Cl… Cl -> z ~ 1000 Cl -> z ~ 1000 Lensing detected ~ 25 σ (after ACT) Lensing detected ~ 25 σ (after ACT) Lensing -> z ~ 2 (consistent with predictions of ∧ CDM…) Lensing -> z ~ 2 (consistent with predictions of ∧ CDM…) A.Benoît-Levy
More CMB than with Planck… More CMB than with Planck…
l < 9000 l < 9000 Fist lensing detection Fist lensing detection SZ Clusters SZ Clusters M.Niemack
More than CMB, with Planck… More than CMB, with Planck…
More than CMB… More than CMB… M.Lopez-Caniego Esquisite full sky mm & sub-mm survey with more than sources
More than CMB… More than CMB… L.Montier New class of objects at high redshift
More than CMB… More than CMB… Tension between CMB and clusters in Planck
More than CMB… More than CMB… Optical data to calibrate the Y-M for SALT B.Kirk
Constraining Inflation - n - running… - r -> B-modes CMB A Window on the early universe J.Martin
Entropic & adiabatic perturbations Scalar power spectrum Gravity waves Non-Gaussianities Single Field slow-roll Single Field with non- canonical kinetic terms Multi field Single Field with Features (ie non slow-roll) Physical Models Observables … … … … J.Martin
ASPIC evidence: good models theory.physics.unige.ch/~ringeval/aspic.html
Physically motivated models can pass present day constraints: - Non linear sigma model (S.Koh) - Heavy field (M.Yamaguchi) Power spectrum. Power spectrum. Isocurvature contribution. Isocurvature contribution. Non Gaussiannity Non Gaussiannity The landscape beyond single field inflation…
Testing Inflation after the Planck era
Sequence is right… Testing Inflation after the Planck era
Sequence is right… Will be painful… Testing Inflation after the Planck era
Primordial non-gaussianity Most inflationary models predict small but model dependent deviations from Gaussianity Primordial non-gaussianity Most inflationary models predict small but model dependent deviations from Gaussianity M.Liguori
Primordial non-gaussianity
Testing anisotropy Y.Fantaye
Testing anisotropy D.Witlshire
… as rulers. R.Triay Using voids…
What is anisotropies play a dynamical role? D.Witlshire, J.Ostrowski
Hunting B-modes… Testing Inflation after the Planck era
And the winners are … KMIII HI J.Martin
And the winners are … J.Martin
Hunting B-modes… M.Lopes-Caniego
Hunting B-modes… M.-A. Bigot-Sazy
Hunting B-modes… H.Nguyen
Hunting B-modes… H.Nguyen
BICEP1,2,3,Keck-Array r = 0.01 is the big game…
Conforting the standard model ( ∧ CDM) Evidencing Dark matter
Evidencing dark matter Accelerator searches Direct detection Indirect detection
Evidencing Dark matter P.Tinyakov
Evidencing Dark matter F. Cafagna
Evidencing Dark matter F. Cafagna
Evidencing Dark matter F. Cafagna
Evidencing Dark matter AMS: Cosmic rays W. Gillard
Evidencing Dark matter DM particle in the room… B. Serfass
Evidencing Dark matter B. Serfass
Evidencing Dark matter N. Kanaya LHC
Evidencing Dark matter N. Kanaya No signal yet… LHC
Dark matter: entering into the controversies… You do not find dark matter because there is dark matter… Debate … M.Milgrom, B.Famey, L.Blanchet
Dark energy: before entering into the controversies… We are all living in an accelerated universe… There is no observational reason to go beyond ∧
Dark energy M.Betoule
Dark energy: galaxy surveys M.Betoule
Dark energy: redshift surveys Boss I, II, III, DESI… S.Bailey
Dark energy: redshift surveys Boss I, II, III, DESI… S.Bailey
Dark energy: redshift surveys Boss I, II, III, DESI… S.Belay
Dark energy: Lα clouds with z ~ 2.3 G.Rossi
Dark energy: the LSST perspective F.Villa
Dark energy: the LSST perspective F.Villa
Dark energy: the LSST perspective F.Villa
Dark energy: the SKA perspective C.Cress
Dark energy: the SKA perspective C.Cress
Dark energy: entering into the controversies… (weak) R.Triay
Dark energy: Nature & Controversies Quantum vacuum ? Quintesssence ? Modified gravity ? Small scale inhomogeneities ? LTB ? A.Blanchard C.Cress D.Whitshire J.Ostrowski
We are waiting for the next conference in Qui Nhon to monitor progresses Conclusion
Thanks to the organisers and specially to Jean Trân Thanh Vân Conclusion