Science from overlapping lensing / spec-z surveys. Chris Blake (Swinburne)

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1 Science from overlapping lensing / spec-z surveys Chris Blake (Swinburne)

2 Probes of the cosmological model How fast is the Universe expanding with time? How fast are structures growing within it?

3 Redshift-space distortions RSD allow spectroscopic galaxy surveys to measure the growth rate of structure infalling galaxies virialized motions coherent flows observer

4 Why combination of lensing and RSD? Sensitive to theories of gravity in complementary ways General perturbations to FRW metric: are metric gravitational potentials, identical in General Relativity but can differ in general theories Relativistic particles (e.g. light rays for lensing) collect equal contributions and are sensitive to Non-relativistic particles (e.g. galaxies infalling into clusters) experience the Newtonian potential

5 Applications arxiv: CFHTLenS: Testing the Laws of Gravity with Tomographic Weak Lensing and Redshift Space Distortions 12 Fergus Simpson 1, Catherine Heymans 1, David Parkinson 2, Chris Blake 3, Martin Kilbinger 4,5,6, Jonathan Benjamin 7, Thomas Erben 8, Hendrik Hildebrandt 7,8, Henk Hoekstra 9,10, Thomas D. Kitching 1, Yannick Mellier 11, Lance Miller 12, arxiv: Confirmation of general relativity on large scales from weak lensing and galaxy velocities 1 Reinabelle Reyes 1, Rachel Mandelbaum 1, Uros Seljak 2-4, Tobias Baldauf 2, James E. Gunn 1, Lucas Lombriser 2, Robert E. Smith 2

6 Overlaps of lensing and spec-z surveys Improvement of cosmological measurements through addition of galaxy-galaxy lensing [e.g. determines bias of lens sample which improves RSD measurements of lenses, especially when using multiple-tracer techniques, e.g. Cai & Bernstein (2012)] Spec-z survey allows definition of lens samples (e.g. groups, galaxy types) enabling a range of studies Understanding, calibration and risk mitigation of systematic errors (photo-z errors including outliers, intrinsic alignments, cosmic shear)

7 Overlaps of lensing and spec-z surveys Mis-match between imaging and spectroscopic surveys!

8 Overlaps of lensing and spec-z surveys w a Many recent 31 July papers 2013 considering impact for cosmology of same-sky vs. different-sky lensing/spec-z surveys !1!2!3!4!5!2!1.5!1!0.5 0 w 0 ee FoM = 1.6 nn FoM = 0.9 ee + nn FoM = 7.2 ee + ne + nn FoM = ee MGFoM 1 INTRODUCTION = 0.3 nn MGFoM = 0.6 For me a key issue is systematic error control ee + The nn MGFoM era of precision = 50.1 cosmology is now a reality. Different arxiv: v1 [astro-ph.co] 30 Jul 2013 Donnacha Kirk 1, Ofer Lahav 1, Sarah Bridle 2, Stephanie Jouvel 3, Filipe B. Abdalla 1, Joshua A. Frieman 4 1 Department of Physics & Astronomy, University College London, Gower Street, London, WC1E 6BT, UK 2 Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, The University of Manchester, Manchester, M13 9PL, UK 3 Institut de Ciències de l Espai (ICE, IEEC/CSIC), E Bellaterra (Barcelona), Spain 4 Fermilab Center for Particle Astrophysics, Batavia, IL Kavli Institute for Cosmological Physics, The University of Chicago, Chicago, IL arxiv: v1 [astro-ph.co] 30 Jul 2013 ABSTRACT The combination of multiple cosmological probes can produce measurements of cosmological parameters much more stringent than those possible with any individual probe. Mon. Not. R. Astron. Soc. 000, 1 21 (2009) Printed 31 July 2013 (MN LATEX style file v2.2) Weon examine deviations the combination from GRof and two highly the arxiv: final correlated jointprobes constraint of late-time withstructure growth: (i) weak gravitational lensing from a survey with photometric redshifts and (ii) cross-correlations galaxy clustering andis redshift over space an order distortions of magnitude from a survey smaller with spectroscopic in redshifts. Optimising termswe of MG choose Spectroscopic FoM generic than survey when designs and RSDs Photometric soare thatincluded. our results Galaxy are applicable to a range Surveys: of In current the Same-sky following and future Benefits photometric sub-sections for redshift we Dark perturb (e.g. Energy KiDS, in turn DES, and ahsc, range Modified Euclid) and spectroscopic redshift (e.g. DESI, 4MOST, Sumire) surveys. Combining the surveys greatly Gravity of the improves assumptions their power wetohave measure made bothfor dark our energy fiducial and modified forecast. gravity. An independent, Some of non-overlapping the results are combination summarised sees ain dark table energy 4 for figure ease of of merit more than Donnacha comparison. 4 times Kirk larger 1, Ofer thanlahav that 1 produced, Sarah Bridle by either 2, Stephanie survey Jouvel alone. 3 The, powerful synergies Filipe between B. Abdalla the surveys 1, Joshua are A. strongest Frieman 4 for modified gravity, where their constraints are 1 Department orthogonal, of Physics producing & Astronomy, University a non-overlapping College London, Gower joint Street, figure London, WC1E of merit 6BT, UKnearly 2 orders of 2 Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, The University of Manchester, Manchester, M13 9PL, UK magnitude larger than either alone. Our projected angular power spectrum formalism 4 Fermilab 3 Institut de Ciències de l Espai (ICE, IEEC/CSIC), E Bellaterra (Barcelona), Spain 5.1 makes Center Survey it for easy Particle toastrophysics, model Specific the Batavia, cross-correlation Target IL Selection observable when the surveys overlap 4 Kavli Institute for Cosmological Physics, The University of Chicago, Chicago, IL on the sky, producing a joint data vector and full covariance matrix. We calculate a same-sky We have improvement assumedfactor, a generic from the survey inclusion strategy of thesefor cross-correlations, our spec-z relative to31 non-overlapping July 2013 surveys. We find nearly a factor of 4 for dark energy and more than a factor survey of 2in for order modified thatgravity. our results The exact might forecast be as widely figures of applicable merit and same-sky benefits as possible. can be radically Another ABSTRACT affected benefit by a range of assuming of forecasts aassumption, constant galaxy which we explore methodically The combination of multiple cosmological probes can produce measurements of cosmological =1.7analysis. parameters that We density out in a to sensitivity z much more our show stringent results that that than those areour possible notfiducial with hostage assumptions any individual probe. produce robust resultswe which examine give the acombination good average of two highly picture correlated of the probes science of late-time return structure from to the particularities of a certain target selection strategy combining photometricgrowth: and spectroscopic (i) weak gravitational surveys. lensing from a survey with photometric redshifts and which could interact (ii) galaxyin clustering a peculiar and redshiftway space distortions with, from foraexample, survey with spectroscopic Key words: cosmology: redshifts. observations We choose generic gravitational survey designs lensing so that our dark results energy are applicable modified to a redshift coverage, range photo-z of current and error futureor photometric k/z-dependence redshift (e.g. KiDS, ofdes, galaxy HSC, Euclid) and gravity cosmological spectroscopic parameters redshift large-scale (e.g. DESI, 4MOST, structure Sumire) of Universe surveys. Combining the surveys bias. greatly improves their power to measure both dark energy and modified gravity. An independent, non-overlapping combination sees a dark energy figure of merit more We recognise thanthat 4 timesno largerindividual than that produced survey by eitheras survey carried alone. Theout powerful synergies between the surveys are strongest for modified gravity, where their constraints will look exactlyare like orthogonal, producing toy survey a non-overlapping we assume joint figurehere. of merit nearly The2 orders of impact of specific magnitudecolless survey largerand than 2003) eitherchronicle target alone. selection Ourthe projected growth strategies angular of cosmic power spectrum structure are formalism makesweak it easy to Gravitational model the cross-correlation Lensing (WGL) observable (Hoekstra when the surveys & Jain overlap 2008; and considered in our on the companion sky, producing a joint paper data vector Jouvel and full (2013). covariance matrix. In this We calculate a same-sky improvement Heymans 2012) factor, from gives theus, inclusion through of these thecross-correlations, bending of light, relative access thetoconstraints surveys. dark matter, We find nearly the of aone dominant factorrepresentative of 4 for matter dark energy species, and more invisible than section we reproduce to non-overlapping a factor of 2 for modified gravity. The exact forecast figures of merit and same-sky survey drawn from benefitsthat to direct can radically paper observation. affected to illustrate by a range of forecasts the assumption, differences which we explore methodically in a sensitivity analysis. We show that that our fiducial assumptions with respect to the produce surveythe robust results model next whichwe decade giveassume will bring a good average here. an picture We even of the choose greater wave of science return from combiningdata photometric as many and spectroscopic of thesesurveys. cosmic probes are scaled up to survey with an exposure time of 20 minutes ee + cosmological ne + nn MGFoM probes = are able to measure some of the most fundamental properties of our Universe from the Cosmic Microwave Background (CMB) (Planck Collaboration et al. 2013; Carlstrom 2011; Sievers 2013) to the type a 5000 deg 2 Ia supernovae (SNe) (Riess 1998; Perlmutter 1999) which chart cover more area on the sky, greater volumes and more ob- Key words: cosmology: observations gravitational 2 lensing dark energy modified

9 Photometric redshift calibration Photometric redshift errors are one of the leading systematics for weak lensing tomography Mean and width of redshift distributions in each photo-z bin must be known to accuracy ~ 10-3 Method (1) : spectroscopic training set [issues : sample variance, incompleteness of training set, outliers] Method (2) : photo-z/spec-z cross-correlations [issues : degeneracies with galaxy bias, cosmic magnification] Can OzDES currently help with either method?

10 Photometric redshift calibration Training set method : suppressing sample variance systematic for DES weak lensing requires 100 AAOmega pointings or 5 VIPERS surveys! Phot-z/spec-z cross-correlation method : need ~50,000 spec-z s per unit redshift -- can use 2dFGRS, SDSS, BOSS at z < 0.6 and VIPERS at z > 0.6? OzDES is not currently transformational for this science, but photo-zs are still useful for other largescale structure topics with less stringent requirements

11 Future AAT proposals? OzDES-wide proposed in March 2013 (150 nights, 3000 deg 2 coverage) - not approved Issue (1) : time now allocated to other projects (SAMI, OzDES-deep) - only nights/semester remain? Issue (2) : can only observe DES fields in B semesters Issue (3) : need to map > 1000 deg 2 to be competitive (e.g. existing RCS2, future HSC projects) Current status : musing on competitiveness of 2014B proposal targetting KiDS, later widening to DES?

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