Testing Dark Energy and Gravity

Slides:



Advertisements
Similar presentations
Weighing Neutrinos including the Largest Photometric Galaxy Survey: MegaZ DR7 Moriond 2010Shaun Thomas: UCL “A combined constraint on the Neutrinos” Arxiv:
Advertisements

1 1 Mapping the History and Fate of the Universe DOE Science Colloquium Eric Linder Lawrence Berkeley National Laboratory.
P ROBING SIGNATURES OF MODIFIED GRAVITY MODELS OF DARK ENERGY Shinji Tsujikawa (Tokyo University of Science)
CMB but also Dark Energy Carlo Baccigalupi, Francesca Perrotta.
Dark Energy and Extended Gravity theories Francesca Perrotta (SISSA, Trieste)
Observational Cosmology - a laboratory for fundamental physics MPI-K, Heidelberg Marek Kowalski.
1 1 Hidden Dimensions, Warped Gravity, Dark Energy Eric Linder UC Berkeley Lawrence Berkeley National Laboratory.
Non-linear matter power spectrum to 1% accuracy between dynamical dark energy models Matt Francis University of Sydney Geraint Lewis (University of Sydney)
Observational Cosmology - a unique laboratory for fundamental physics Marek Kowalski Physikalisches Institut Universität Bonn.
Lecture 2: Observational constraints on dark energy Shinji Tsujikawa (Tokyo University of Science)
Cosmology Zhaoming Ma July 25, The standard model - not the one you’re thinking  Smooth, expanding universe (big bang).  General relativity controls.
CMB as a physics laboratory
Complementary Probes ofDark Energy Complementary Probes of Dark Energy Eric Linder Berkeley Lab.
Quintessence – Phenomenology. How can quintessence be distinguished from a cosmological constant ?
1 What is the Dark Energy? David Spergel Princeton University.
COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.
1 1 Dark Energy in Dark Antarctica Dark Energy in Dark Antarctica Eric Linder 21 July 2009 Berkeley Center for Cosmological Physics, UC Berkeley & Berkeley.
1 1 Eric Linder October 2011 UC Berkeley & Berkeley Lab Institute for the Early Universe Ewha University, Korea ★ ★ GR. Chasing Down Cosmic Acceleration.
Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010.
1 1 Eric Linder 27 June 2012 Testing Dark Energy and Gravity with Cosmological Surveys UC Berkeley & Berkeley Lab Institute for the Early Universe, Korea.
Weak Lensing 3 Tom Kitching. Introduction Scope of the lecture Power Spectra of weak lensing Statistics.
1 1 Eric Linder 7 June 2012 UC Berkeley & Berkeley Lab ★ ★ GR. Chasing Down Cosmic Acceleration.
The Science Case for the Dark Energy Survey James Annis For the DES Collaboration.
Cosmological Tests using Redshift Space Clustering in BOSS DR11 (Y. -S. Song, C. G. Sabiu, T. Okumura, M. Oh, E. V. Linder) following Cosmological Constraints.
Eric V. Linder (arXiv: v1). Contents I. Introduction II. Measuring time delay distances III. Optimizing Spectroscopic followup IV. Influence.
Polarization-assisted WMAP-NVSS Cross Correlation Collaborators: K-W Ng(IoP, AS) Ue-Li Pen (CITA) Guo Chin Liu (ASIAA)
1 1 Eric Linder 21 December 2011 UC Berkeley & Berkeley Lab Institute of the Early Universe, Korea The Direction of Gravity.
Modern State of Cosmology V.N. Lukash Astro Space Centre of Lebedev Physics Institute Cherenkov Conference-2004.
Dark energy I : Observational constraints Shinji Tsujikawa (Tokyo University of Science)
1 1 Eric Linder 24 July 2013 Chasing Down Cosmic Acceleration UC Berkeley & Berkeley Lab Institute for the Early Universe, Korea.
Relic Neutrinos, thermal axions and cosmology in early 2014 Elena Giusarma arXiv: Based on work in collaboration with: E. Di Valentino, M. Lattanzi,
How can CMB help constraining dark energy? Licia Verde ICREA & Institute of space Sciences (ICE CSIC-IEEC)
1 1 Eric Linder University of California, Berkeley Lawrence Berkeley National Lab Interpreting Dark Energy JDEM constraints.
The dark universe SFB – Transregio Bonn – Munich - Heidelberg.
PHY306 1 Modern cosmology 4: The cosmic microwave background Expectations Experiments: from COBE to Planck  COBE  ground-based experiments  WMAP  Planck.
Michael Doran Institute for Theoretical Physics Universität Heidelberg Time Evolution of Dark Energy (if any …)
Ignacy Sawicki Université de Genève Understanding Dark Energy.
Using Baryon Acoustic Oscillations to test Dark Energy Will Percival The University of Portsmouth (including work as part of 2dFGRS and SDSS collaborations)
1 1 The Darkness of the Universe: The Darkness of the Universe: The Heart of Darkness Eric Linder Lawrence Berkeley National Laboratory.
 Acceleration of Universe  Background level  Evolution of expansion: H(a), w(a)  degeneracy: DE & MG  Perturbation level  Evolution of inhomogeneity:
1 1 The Darkness of the Universe: The Darkness of the Universe: Mapping Expansion and Growth Eric Linder Lawrence Berkeley National Laboratory.
1 1 Eric Linder 22 November 2010 UC Berkeley & Berkeley Lab Institute for the Early Universe Ewha University, Korea CMB Probes of Dark Energy.
The dark side of the Universe: dark energy and dark matter Harutyun Khachatryan Center for Cosmology and Astrophysics.
Astro-2: History of the Universe Lecture 10; May
Latest Results from LSS & BAO Observations Will Percival University of Portsmouth StSci Spring Symposium: A Decade of Dark Energy, May 7 th 2008.
Jochen Weller XLI Recontres de Moriond March, 18-25, 2006 Constraining Inverse Curvature Gravity with Supernovae O. Mena, J. Santiago and JW PRL, 96, ,
Dark Energy and baryon oscillations Domenico Sapone Université de Genève, Département de Physique théorique In collaboration with: Luca Amendola (INAF,
Observational evidence for Dark Energy
1 1 Dark Energy with SNAP and other Next Generation Probes Eric Linder Berkeley Lab.
Probing Dark Energy with Cosmological Observations Fan, Zuhui ( 范祖辉 ) Dept. of Astronomy Peking University.
Cheng Zhao Supervisor: Charling Tao
The Nature of Dark Energy David Weinberg Ohio State University Based in part on Kujat, Linn, Scherrer, & Weinberg 2002, ApJ, 572, 1.
Map-making leads to understanding When we understand the evolution from one map to another, we can understand  the sociological, economic, and political.
The Dark Side of the Universe L. Van Waerbeke APSNW may 15 th 2009.
* The collection of powerful ideas formerly known as String Theory Dark Energy: 2020 Vision DPF SNOWMISS SLAC Cosmic Frontier Workshop 6 to 8 March 2013.
Dark Energy From the perspective of an American theorist fresh from the recent Dark Energy Survey Collaboration Meeting Scott Dodelson.
University of California, Berkeley Lawrence Berkeley National Lab
The clustering of galaxies in the completed SDSS-III Baryon Oscillation Spectroscopic Survey : cosmological analysis of the DR12 galaxy sample arXiv:
Princeton University & APC
University of California, Berkeley Lawrence Berkeley National Lab
Probing the Coupling between Dark Components of the Universe
Recent status of dark energy and beyond
Cosmology with Supernovae
University of California, Berkeley Lawrence Berkeley National Lab
Cosmology from Large Scale Structure Surveys
Shintaro Nakamura (Tokyo University of Science)
Ignacy Sawicki CEICO, Institute of Physics, Prague
The impact of non-linear evolution of the cosmological matter power spectrum on the measurement of neutrino masses ROE-JSPS workshop Edinburgh.
Measurements of Cosmological Parameters
6-band Survey: ugrizy 320–1050 nm
Presentation transcript:

Testing Dark Energy and Gravity Eric Linder 17 June2011 ★ GR . UC Berkeley & LBNL Institute for the Early Universe Ewha University, Korea

Describing Our Universe New Stuff Old New Stuff Us STScI 95% of the universe is unknown! Now entertain conjecture of a time When creeping murmur and the poring dark Fills the wide vessel of the universe. - Shakespeare, Henry V, act IV

Cosmic Coincidence Why not just settle for a cosmological constant ?  For 90 years we have tried to understand why  is at least 10120 times smaller than we would expect – and failed.  We know there was an epoch of time varying vacuum once – inflation. We cannot calculate the vacuum energy to within 10120. But it gets worse: Think of the energy in  as the level of the quantum “sea”. At most times in history, matter is either drowned or dry. Size=1/4 Size=1/2 Matter Dark energy Today Size=2 Size=4

On Beyond ! “You’ll be sort of surprised what there is to be found Once you go beyond  and start poking around.” – Dr. Seuss, à la “On Beyond Zebra” New quantum physics? Does nothing weigh something? Einstein’s cosmological constant, Quintessence, String theory New gravitational physics? Is nowhere somewhere? Quantum gravity, extended gravity, extra dimensions? We need to explore further frontiers in high energy physics, gravitation, and cosmology.

Dark Energy as a Teenager 13 years after discovery of the acceleration of the universe, where are we? From 60 Supernovae Ia at cosmic distances, we now have ~600 published distances, with better precision, better accuracy, out to z=1.75. CMB plus external data (H0) points to acceleration. (Didn’t even have acoustic peak in 1998.) BAO detected. Concordant with acceleration. Weak lensing detected. Concordant with acceleration. Cluster masses (if asystematic) ~1.5 for acceleration. Strong concordance among data: DE~0.73, w~-1.

Supernova Properties Astrophysics Understanding Supernovae Supernova Properties Astrophysics Nearby Supernova Factory 400 SN Ia with spectra, z=0.03-0.08 >3000 spectra of SN Ia Cleanly understood astrophysics leads to cosmology (and astrophysics!) G. Aldering (LBL)

Improving Supernovae EW of supernova spectral features can separate color variation and dust extinction. Chotard++ 1103.5300 A&A Letters 2011

Latest Data Union2.1 SN Set Suzuki et al, 1105.3470 Suzuki et al, arXiv:1105.3470 Union2.1 SN Set Complete SALT2 reanalysis, refitting 17 data sets 580 SNe Ia (166+414) - new z>1 SN, HST recalib Fit Mi between sets and between low-high z Study of set by set deviations (residuals, color) Blind cosmology analysis! Systematic errors as full covariance matrix Suzuki et al, ApJ 2011, arXiv:1105.3470

Are We Done? (stat+sys) w(z)? z>1? There is a long way to go still to say we have measured dark energy!

Dark Energy + 13 13 years after today, where will we be? CMB: Planck data, ground based polarization and CMB lensing BAO: BOSS (on sky), WiggleZ, SuMIRe, HETDEX… Full power spectrum (redshift space distortions) Clusters: SZ Effects - ACT, SPT Supernovae: smarter, not just more Multiprobe: DES, KDUST? (Dome A), GSMT? Euclid? LSST? WFIRST? (EuFIRST, USlater?) Stage IV from the ground – BigBOSS?

Higher Dimensional Data Cosmological Revolution: Cosmology is growing in new, sophisticated directions, and data interpretation, synthesis, and visualization will play key roles and deliver unprecedented opportunities to understand the universe and fundamental physics.  From 2D to 3D – CMB anisotropies to tomographic surveys of density/velocity field.

Data, Data, Data As wonderful as the CMB is, it is 2-dimensional. The number of modes giving information is l(l+1) or ~10 million. BOSS (SDSS III) will map 400,000 linear modes. BigBOSS will map 15 million linear modes. N. Padmanabhan conformal diagram SDSS I, II, 2dF BigBOSS: Ground-Based Stage IV Dark Energy Experiment BOSS (SDSS III) BigBOSS 18 million galaxies z=0.2-1.5 600,000 QSOs z=1.8-3 courtesy of David Schlegel

Cosmic Structure Galaxy 3D distribution or power spectrum contains information on: Growth - evolving amplitude Matter/radiation density, H - peak turnover Distances - baryon acoustic oscillations Growth rate - redshift space distortions Neutrino mass, non-Gaussianity, gravity, etc. BigBOSS: initial approval for Kitt Peak/NOAO 4m. arXiv:1106.1706 ; http://bigboss.lbl.gov

Weak Lensing Data systematics Theory systematics Berkeley Weak Lensing code (soon public) Das, de Putter, Linder, Nakajima 1102.5090

Future of Dark Energy Today we know the dark energy equation of state, constant w to ~10%. Future experiments look bright for dark physics. We must test for varying w (no real theory predicts constant w). If w(a) ~ -1, is  the conclusion? No! Many, diverse physics theories give w(a)~-1. Approaching : Microphysics, High Energy Physics, Gravity.

 Attractor from High Energy Physics Quintessence suffers from HEP corrections and fine tuning. DBI action is relativistic generalization solving both. w=-1 in past, and attracted toward w~-1 in future. So today, not so far from w=-1. V, T are brane properties. Deviation from w=-1 related to “mass” 2=(V/T)Pl. Ahn, Kim, & Linder 2009a,b Two interesting signatures: sound speed cs≠1 and early dark energy (dilaton, scaling) DE(z=103)>>(z=103)=10-9.

The Speed of Dark Current constraints on cs using CMB (WMAP5), CMB × gal (2MASS,SDSS,NVSS), gal (SDSS). Future constraints from Planck or CMBpol de Putter, Huterer, Linder 2010 Calabrese++ 2011 cf Joudaki&Kaplinghat ★ Best fit Ωe=0.02, cs=0.04, w0=-0.95 but consistent with  within 68% cl.

CMB Probes of Acceleration How well do we really know the standard picture of radiation domination  matter domination  dark energy domination?Maybe acceleration is occasional. (Solve coincidence) Effect of 0.1 e-fold of acceleration Post-recombination, peaks  left and adds ISW. Pre-recombination, peaks  right and adds SW. Current acceleration unique within last factor 100,000 of cosmic expansion! Linder & Smith 2010

CMB Lensing CMB lensing alone now sees 3.2σ evidence for . Sherwin++ 1105.0419 ACT

Testing Gravity Test gravity in model independent way. Gravity and growth: Gravity and acceleration: Are  and  the same? (yes, in GR) Use relativistic / nonrelativistic geodesic parameters: G relates the metric to the density (Poisson+ eq); central to ISW and lensing. V relates the metric to the motion (velocity/growth eq); central to growth ( closely related).

Model independent “2 x 2 x 2 gravity” Future Data Leverage Model independent “2 x 2 x 2 gravity” low k, low z low k, high z BigBOSS (gg) + Planck CMB + Space SN high k, high z high k, low z Daniel & Linder 2010 cf Song+, Zhao+ Factor of 10-100 improvement; 5-10% test of 8 parameters of model-independent gravity.

Gravity Requirement Look at V-V  phase space dynamics, just like for w-w of dark energy. Today, ΔV~±0.3 and have gravity requirement: 3σ measure requires σ(V)~0.1. ★ GR . Linder 1103.0282

Summary Exciting new data from SN, CMB, LSS. BigBOSS can give 3D map to z<1.5 from ground. Approaching  is very natural from a wide variety of physics - microphysics (barotropic), high energy physics (DBI string theory), gravity (f(R)) - and does not default to . Deviations from  testable with variety of probes, including sound speed and early dark energy. Absolute requirement on testing gravity – 10% on V. Expansion history can be tested to z~105. Current acceleration appears unique! “World Class University” program in Seoul, Korea. Berkeley+ Ewha U.