cosmology surveys (a non-wht talk)

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Cosmology Surveys (a non-WHT talk) Ofer Lahav University College London - Dark Energy science and beyond - Imaging surveys - Spectroscopic surveys

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Cosmology Surveys (a non-WHT talk). Ofer Lahav University College London. D a rk Energy science and beyond Imaging surveys - Spectroscopic surveys. “Evidence” for Dark Energy. Observational data Type Ia Supernovae Galaxy Clusters Cosmic Microwave Background - PowerPoint PPT Presentation

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Page 1: Cosmology Surveys (a non-WHT talk)

Cosmology Surveys(a non-WHT talk)

Ofer Lahav University College London

- Dark Energy science and beyond- Imaging surveys- Spectroscopic surveys

Page 2: Cosmology Surveys (a non-WHT talk)

“Evidence” for Dark Energy

Observational data• Type Ia Supernovae • Galaxy Clusters• Cosmic Microwave Background• Large Scale Structure• Gravitational Lensing• Integrated Sachs-Wolfe

Physical effects: • Geometry • Growth of StructureBoth depend on the Hubble expansion rate:

H2(z) = H20 [M (1+z) 3 + DE (1+z) 3 (1+w) ] (flat)

Page 3: Cosmology Surveys (a non-WHT talk)

Dark Energy Pre-SNIa

• Peebles (1984) advocated Lambda

• APM result for low matter density (Efstathiou et al. 1990)

• Baryonic fraction in clusters (White et al. 1993)

• The case for adding Lambda (Ostriker & Steinhardt 1995)

• Others…

Calder & OL, Physics World, Jan 2010

Page 4: Cosmology Surveys (a non-WHT talk)

What will be the next paradigm shift?

• Vacuum energy (cosmological constant)?• Dynamical scalar field?

– w=p/– for cosmological constant: w = -1

• Manifestation of modified gravity?• Inhomogeneous Universe?

• What if cosmological constant after all?• Multiverse - Landscape?• The Anthropic Principle?

Page 5: Cosmology Surveys (a non-WHT talk)

Standard rulers

Page 6: Cosmology Surveys (a non-WHT talk)

Baryonic Acoustic Oscillations

SDSS Luminous Red GalaxiesDensity fluctuations

CMB WMAPTemperature fluctuations

Comving distance Harmonic l

z=0.5 z=1000

Page 7: Cosmology Surveys (a non-WHT talk)

Probing the Geometryof the Universe with

Supernovae Ia

‘Union’ SN Ia sample (Kowalski et al. 2008)

Page 8: Cosmology Surveys (a non-WHT talk)

In 3 Dimensions

Massey et al. 2007

Page 9: Cosmology Surveys (a non-WHT talk)

Galaxy Surveys2010-2020

Photometric surveys: DES, Pan-STARRS, HSC, Skymapper, PAU, LSST, Euclid (EIC), JDEM(SNAP-like), …

Spetroscopic surveys: WiggleZ, BOSS, BigBOSS, hetdex, WFMOS/Sumire, Euclid (NIS) JDEM (Adept-like), SKA, …

Page 10: Cosmology Surveys (a non-WHT talk)

Photometric redshifts

• Probe strong spectral features (e.g. 4000 break)

• Template vs. Training methods

z=3.7z=0.1

Page 11: Cosmology Surveys (a non-WHT talk)

MegaZ-LRG

• Input: 10,000 galaxies with spectra

• Train a neural network

•ANNz, Collister & Lahav 2004

• Output: 1,000,000 photo-z•Collister, Lahav et al. 2007

•Update using 6 photo-z methods *Abdalla et al. 2009

3 (Gpc/h)3: the largest ever galaxy redshift survey!

Photoz scatter of 0.04

Page 12: Cosmology Surveys (a non-WHT talk)

Neutrino mass from MegaZ-LRG

Thomas, Abdalla & OL (2009) 0911.5291

Total mass < 0.3 eV (95% CL)

Page 13: Cosmology Surveys (a non-WHT talk)

The Dark Energy http://www.darkenergysurvey.org

Page 14: Cosmology Surveys (a non-WHT talk)

The DES Collaborationan international collaboration of ~100 scientists from ~20 institutions

US: Fermilab, UIUC/NCSA, University of Chicago,LBNL, NOAO, University of Michigan, University of Pennsylvania, Argonne National Laboratory, Ohio State University, Santa-Cruz/SLAC Consortium

Observatorio Nacional, CBPF,Universidade Federal do Rio de Janeiro, Universidade Federal do Rio Grande do Sul

Brazil Consortium:

UK Consortium:UCL, Cambridge, Edinburgh, Portsmouth, Sussex, Nottingham

Spain Consortium:CIEMAT, IEEC, IFAE

CTIO

Page 15: Cosmology Surveys (a non-WHT talk)

The Dark Energy Survey (DES)• Proposal:

– Perform a 5000 sq. deg. survey of the southern galactic cap

– Measure dark energy with 4 complementary techniques

• New Instrument:– Replace the PF cage with a

new 2.2 FOV, 520 Mega pixel optical CCD camera + corrector

• Time scale:– Instrument Construction

2008-2011• Survey:

– 525 nights during Oct.–Feb. 2011-2016

– Area overlap with SPT SZ survey and VISTA VHS

Use the Blanco4m Telescope at the Cerro TololoInter-American Observatory (CTIO)

Page 16: Cosmology Surveys (a non-WHT talk)

The 5 lenses are now being polished

C2

Polishing & coating coordinated by UCL (with 1.7M STFC funding)

C1

Page 17: Cosmology Surveys (a non-WHT talk)

Galactic Plane

Deep~40 deg2

Wide Extragalactic20,000 deg2

Euclid Imaging SurveysWide Survey: Extragalactic sky (20,000 deg2 = 2 sr)

• Visible: Galaxy shape measurements to RIZAB ≤ 24.5 (AB, 10σ) at 0.16” FWHM, yielding 30-40 resolved galaxies/amin2, with a median redshift z~ 0.9

• NIR photometry: Y, J, H ≤ 24 (AB, 5σ PS), yielding photo-z’s errors of 0.03-0.05(1+z) with ground based complement (PanStarrs-2, DES. etc)

• Concurrent with spectroscopic survey

Deep Survey: 40 deg2 at ecliptic poles

•Monitoring of PSF drift (40 repeats at different orientations over life of mission)

•Produces +2 magnitude in depth for both visible and NIR imaging data.

Possible additional Galactic surveys:

•Short exposure Galactic plane•High cadence microlensing extra-solar planet surveys could be easily added within Euclid mission architecture.

Page 18: Cosmology Surveys (a non-WHT talk)

Spectroscopic Surveys

CfA

SDSS

2dFGRS

2MRS

Page 19: Cosmology Surveys (a non-WHT talk)

SUBARU:the ups and downs of WFMOS

and the hopes for SUMIRE

Page 20: Cosmology Surveys (a non-WHT talk)

Redshift Distortion as a test of Modified Gravity

Guzzo et al. 2008

Page 21: Cosmology Surveys (a non-WHT talk)

BigBOSS: The Ground-Based Stage IV BAO Experiment

• http://bigboss.lbl.gov/

A new 5000-fiber R=5000 spectrograph covering a 3-degree diameter field will measure BAO and redshift space distortions in the distribution of galaxies and hydrogen gas spanning redshifts from 0.2 < z < 3.5. The Dark Energy Task Force figure of merit (DETF FoM) for this experiment is expected to be equal to that of a JDEM mission for BAO with the lower risk and cost typical of a ground-based experiment

Page 22: Cosmology Surveys (a non-WHT talk)

Cosmology Surveys - summary

* Goal: Dark Energy parameters

to a few % level

• Both imaging and spectroscopy surveys are essential

• Is a BAO survey with a 4m feasible?

• Non-DE science with DE surveys

(e.g. Neutrino mass, galaxy evolution,

MW structure, QSOs)

Page 23: Cosmology Surveys (a non-WHT talk)

THE END

Page 24: Cosmology Surveys (a non-WHT talk)

Planned photometric and spectroscopic surveys

Page 25: Cosmology Surveys (a non-WHT talk)

The Dark Energy problem: 10, 90 or 320 years old?The weak field limit of GR:F = -GM/r2 + /3 r

X *

Lucy Calder & OLA&G Feb 08 issuehttp://www.star.ucl.ac.uk/~lahav/CLrev.pdf (revised)

“I have now explained the TWO principle cases of attraction…which is very remarkable” Isaac Newton, Principia (1687)

Page 26: Cosmology Surveys (a non-WHT talk)

Dark Energy Science ProgramFour Probes of Dark Energy• Galaxy Clusters

• clusters to z>1• SZ measurements from SPT• Sensitive to growth of structure and geometry

• Weak Lensing• Shape measurements of 300 million galaxies • Sensitive to growth of structure and geometry

• Large-scale Structure• 300 million galaxies to z = 1 and beyond• Sensitive to geometry

• Supernovae• 15 sq deg time-domain survey• ~3000 well-sampled SNe Ia to z ~1• Sensitive to geometry

Plus QSOs, Strong Lensing, Milky Way, Galaxy Evolution

Page 27: Cosmology Surveys (a non-WHT talk)

DES Forecasts: Power of Multiple Techniques

FoM factor 4.6 tigther compared to near term projects

w(z) =w0+wa(1–a) 68% CL

Page 28: Cosmology Surveys (a non-WHT talk)

The Chequered History of theCosmological Constant

* The old CC problem:Theory exceeds observational limits on by 10120 !

* The new CC problem:Why are the amounts of Dark Matter and Dark Energy so similar?

Page 29: Cosmology Surveys (a non-WHT talk)
Page 30: Cosmology Surveys (a non-WHT talk)

Photo-z –Dark Energy cross talk

• Approximately, for a photo-z slice:

(w/ w) = 5 (z/ z) = 5 (z/z) Ns-1/2

=> the target accuracy in w

and photo-z scatter z dictate the number of required spectroscopic redshifts

Ns =105-106

Page 31: Cosmology Surveys (a non-WHT talk)

Euclid - impact on Cosmology

Euclid Imaging will challenge all sectors of the cosmological model:

• Dark Energy: wp and wa with an error of 2% and 13% respectively (no prior)

• Dark Matter: test of CDM paradigm, precision of 0.04eV on sum of neutrino masses (with Planck)

• Initial Conditions: constrain shape of primordial power spectrum, primordial non-gaussianity

• Gravity: test GR by reaching a precision of 2% on the growth exponent (dlnm/dlnam

)

Uncover new physics and Map LSS at 0<z<2: Low redshift counterpart to CMB surveys

Δwp ΔWa ΔΩm ΔΩΛ ΔΩb Δσ8 Δns Δh DE FoM

Current+WMAP 0.13 - 0.01 0.015 0.0015 0.026 0.013 0.013 ~10

Planck - - 0.008 - 0.0007 0.05 0.005 0.007 -

Weak Lensing 0.03 0.17 0.006 0.04 0.012 0.013 0.02 0.1 180

Imaging Probes 0.018 0.15 0.004 0.02 0.007 0.0009 0.014 0.07 400

Euclid 0.016 0.13 0.003 0.012 0.005 0.003 0.006 0.020 500

Euclid +Planck 0.01 0.066 0.0008 0.003 0.0004 0.0015 0.003 0.002 1500

Factor Gain 13 >15 13 5 4 17 4 7 150