Elise Jennings University of Chicago

Similar documents
CosmoSIS a statistical framework for precision cosmology. Elise Jennings

Testing General Relativity with Redshift Surveys

BAO & RSD. Nikhil Padmanabhan Essential Cosmology for the Next Generation VII December 2017

N-body Simulations and Dark energy

The quest for Dark Energy when theories meet simulations

Beyond BAO: Redshift-Space Anisotropy in the WFIRST Galaxy Redshift Survey

Cosmology with high (z>1) redshift galaxy surveys

Baryon Acoustic Oscillations and Beyond: Galaxy Clustering as Dark Energy Probe

The Power. of the Galaxy Power Spectrum. Eric Linder 13 February 2012 WFIRST Meeting, Pasadena

Takahiro Nishimichi (IPMU)

The Dark Sector ALAN HEAVENS

Énergie noire Formation des structures. N. Regnault C. Yèche

Large Scale Structure with the Lyman-α Forest

The large scale structure of the universe

BARYON ACOUSTIC OSCILLATIONS. Cosmological Parameters and You

What can Cosmology tell us about Gravity? Levon Pogosian Simon Fraser University

Precision Cosmology from Redshift-space galaxy Clustering

Redshift Space Distortion Introduction

Diving into precision cosmology and the role of cosmic magnification

Cosmology Beyond the Standard Model

redshift surveys Kazuhiro Yamamoto T. Sato (Hiroshima) G. Huetsi (UCL) 2. Redshift-space distortion

Cosmology with Peculiar Velocity Surveys

BAO & RSD. Nikhil Padmanabhan Essential Cosmology for the Next Generation December, 2017

Introduction to CosmoMC

Physical Cosmology 4/4/2016. Docente: Alessandro Melchiorri

Basic BAO methodology Pressure waves that propagate in the pre-recombination universe imprint a characteristic scale on

Galileon Cosmology ASTR448 final project. Yin Li December 2012

New Probe of Dark Energy: coherent motions from redshift distortions Yong-Seon Song (Korea Institute for Advanced Study)

Effective Field Theory approach for Dark Energy/ Modified Gravity. Bin HU BNU

Dark Energy in Light of the CMB. (or why H 0 is the Dark Energy) Wayne Hu. February 2006, NRAO, VA

New techniques to measure the velocity field in Universe.

Cosmological Constraints from Redshift Dependence of Galaxy Clustering Anisotropy

Recent BAO observations and plans for the future. David Parkinson University of Sussex, UK

Beyond ΛCDM: Dark energy vs Modified Gravity

Non-Standard Cosmological Simulations

Consistent modified gravity analysis of anisotropic galaxy clustering using BOSS DR11

Baryon Acoustic Oscillations Part I

Cosmology and Large Scale Structure

Concordance Cosmology and Particle Physics. Richard Easther (Yale University)

A5682: Introduction to Cosmology Course Notes. 11. CMB Anisotropy

Un-natural aspects of standard cosmology. John Peacock Oxford anthropics workshop 5 Dec 2013

Constraining Modified Gravity and Coupled Dark Energy with Future Observations Matteo Martinelli

The State of Tension Between the CMB and LSS

Physics of the Large Scale Structure. Pengjie Zhang. Department of Astronomy Shanghai Jiao Tong University

Galaxies 626. Lecture 3: From the CMBR to the first star

What do we really know about Dark Energy?

CONSTRAINTS AND TENSIONS IN MG CFHTLENS AND OTHER DATA SETS PARAMETERS FROM PLANCK, INCLUDING INTRINSIC ALIGNMENTS SYSTEMATICS. arxiv:1501.

COSMOLOGY CURRENT SURVEYS AND INSTRUMENTATION MATTHEW COLLESS MULTI-OBJECT SPECTROSCOPY IN THE NEXT DECADE SANTA CRUZ DE LA PALMA

A5682: Introduction to Cosmology Course Notes. 11. CMB Anisotropy

arxiv: v4 [astro-ph.co] 24 Mar 2015

Are VISTA/4MOST surveys interesting for cosmology? Chris Blake (Swinburne)

Simulating non-linear structure formation in dark energy cosmologies

Results from the Baryon Oscillation Spectroscopic Survey (BOSS)

Fundamental cosmology from the galaxy distribution. John Peacock Hiroshima 1 Dec 2016

Is inflation really necessary in a closed Universe? Branislav Vlahovic, Maxim Eingorn. Please see also arxiv:

Dark Energy and Dark Matter Interaction. f (R) A Worked Example. Wayne Hu Florence, February 2009

Theoretical developments for BAO Surveys. Takahiko Matsubara Nagoya Univ.

Observational evidence for Dark energy

TESTING GRAVITY WITH COSMOLOGY

Measuring Neutrino Masses and Dark Energy

CosmoSIS Webinar Part 1

The impact of relativistic effects on cosmological parameter estimation

Observational cosmology: the RENOIR team. Master 2 session

EUCLID Cosmology Probes

Large Scale Structure After these lectures, you should be able to: Describe the matter power spectrum Explain how and why the peak position depends on

Signatures of MG on. linear scales. non- Fabian Schmidt MPA Garching. Lorentz Center Workshop, 7/15/14

H 0 is Undervalued BAO CMB. Wayne Hu STSCI, April 2014 BICEP2? Maser Lensing Cepheids. SNIa TRGB SBF. dark energy. curvature. neutrinos. inflation?

Absolute Neutrino Mass from Cosmology. Manoj Kaplinghat UC Davis

Modern Cosmology / Scott Dodelson Contents

Mario Santos (on behalf of the Cosmology SWG) Stockholm, August 24, 2015

Mapping the dark universe with cosmic magnification

The rise of galaxy surveys and mocks (DESI progress and challenges) Shaun Cole Institute for Computational Cosmology, Durham University, UK

Cosmology and dark energy with WFIRST HLS + WFIRST/LSST synergies

A Framework for. Modified Gravity. Models of Cosmic Acceleration. Wayne Hu EFI, November 2008

Parameterizing. Modified Gravity. Models of Cosmic Acceleration. Wayne Hu Ann Arbor, May 2008

A look into the Dark Universe

BAO and Lyman-α with BOSS

Let me introduce myself...

Cosmology. Introduction Geometry and expansion history (Cosmic Background Radiation) Growth Secondary anisotropies Large Scale Structure

CONSTRAINTS AND TENSIONS IN MG CFHTLENS AND OTHER DATA SETS PARAMETERS FROM PLANCK, INCLUDING INTRINSIC ALIGNMENTS SYSTEMATICS.

Baryon acoustic oscillations A standard ruler method to constrain dark energy

Measuring the Cosmic Distance Scale with SDSS-III

Late time cosmology with GWs

Testing gravity on Large Scales

Unication models of dark matter and dark energy

Modified gravity as an alternative to dark energy. Lecture 3. Observational tests of MG models

Cosmology with the ESA Euclid Mission

Neutrinos in the era of precision Cosmology

The Principal Components of. Falsifying Cosmological Paradigms. Wayne Hu FRS, Chicago May 2011

Toward a Parameterized Post Friedmann. Description of Cosmic Acceleration

2013: A Good Year for Cosmology A Brief History of Contemporary Cosmology

Determining neutrino masses from cosmology

Cosmological Constraints on Dark Energy via Bulk Viscosity from Decaying Dark Matter

arxiv: v1 [astro-ph.co] 3 Apr 2019

Constraining Dark Energy and Modified Gravity with the Kinetic SZ effect

A FIGURE OF MERIT ANALYSIS OF CURRENT CONSTRAINTS ON TESTING GENERAL RELATIVITY USING THE LATEST COSMOLOGICAL DATA SETS.

Cosmic Acceleration from Modified Gravity: f (R) A Worked Example. Wayne Hu

Detecting Dark Energy Perturbations

Brief Introduction to Cosmology

Testing gravity on cosmological scales with the observed abundance of massive clusters

Transcription:

Pacific 2014 Testing gravity with large scale structure dynamics Elise Jennings University of Chicago THE UNIVERSITY OF CHICAGO THE ENRICO FERMI INSTITUTE

EJ, B. Li, C.M. Baugh, G. Zhao, K. Kazuya 2013 EJ 2012 EJ, C. M. Baugh, S. Pascoli 2011 Outline Accelerating expansion Growth of structure & Expansion history Redshift space distortions : an important cosmological probe Measuring the growth rate: Dark energy vs. modified gravity

Probing Dark Energy Supernovae, CMB BAO, Weak Lensing & Cluster observations ΛCDM cosmology Ω TOTAL ~ 1 ~25% Dark Matter ~75% Dark Energy What is causing the accelerating expansion? Is dark energy constant or does it evolve with time? General Relativity or Modified gravity? Missions to study the dark sector need precise measurements: Expansion history H(z) Growth rate f= dlnd/dlna

Probing Dark Energy WiggleZ BOSS DES EUCLID WFIRST eboss PFS DESI HETDEX LSST BAO, Pk/ξ, SN 0.5<z<0.9 Weak lensing shear signal, clusters, SN BAO, Pk/ξ, SN 1<z<3 0.6<z<1 0.8<z<2.4 0.6<z<1.5, quasers 1<x<3.5 Goal: Measure the growth rate to 1% over 0.25<z<3 Expansion rate to <1%

N-body simulations are an essential tool - Model nonlinear fluctuation growth, peculiar motions, nonlinear and scale dependent bias - Study nonlinear growth in different cosmologies Angulo et al. 2008

Redshift space distortions Real space Redshift space Large scales: Galaxies undergoing infall towards a spherical overdensity : shell appears squashed.

Redshift space distortions Real space Redshift space Large scales: Galaxies undergoing infall towards a spherical overdensity : shell appears squashed. Small scales: Incoherent peculiar motions giving rise to fingers-of-god.

The Dark Energy Science report aka Rocky III : RSD among the most powerful ways of addressing whether the acceleration is caused by dark energy or modified gravity" Power spectrum in redshift space Linear theory Growth rate Linear bias

Current measurements & forecasts Blake et al 2011 z=0.57: fσ 8 (a) = 0.43 ± 0.07 Reid et al. 2012 Majerotto et al. 2012

Power spectrum in linear theory 2 Growth rate Linear bias Correlation function Kaiser (1987)

Improved model for the redshift space P(k): Velocity divergence cross P(k) Velocity divergence auto P(k) On what scales is the linear continuity equation valid? k (h/mpc)

Improved model for the redshift space P(k): Velocity divergence cross P(k) Velocity divergence auto P(k) On what scales is the linear continuity equation valid? k (h/mpc)

Blake et al. 2011

Dark Energy or modified gravity Anything that can simultaneously explain Angular diameter distances (BAO, CMB) Luminosity distances (Supernovae Ia) can be called dark energy but could be the result of modified gravity Measuring the expansion history alone will not distinguish modified gravity from smooth dark energy Need to break the degeneracy with measurements of growth factor

Dark energy e.g Quintessence Modified gravity e.g. parametrised by µ 2 = G/G N and ζ = 1-Ψ/Φ slip parameter

Dark energy e.g Quintessence Within GR growth of density perturbations grows according to Modified gravity e.g. parametrised by µ 2 = G/G N and ζ = 1-Ψ/Φ slip parameter If gravitational constant varies & g = δ/a

Dark energy e.g Quintessence Within GR growth of density perturbations grows according to Modified gravity e.g. parametrised by µ 2 = G/G N and ζ = 1-Ψ/Φ slip parameter If gravitational constant varies & g = δ/a Consistency test of cosmology : compare growth & expansion rates Growth rate Growth rate

GR real space GR redshift space Simulations: Modified Ramses Two D pic GR f4 f(r) real space f(r) redshift space EJ, Baugh, Li, Zhao & Koyama 2012

f R0 =10-5 f R0 =10-4 P_tt/P_dd Linear theory f(r) Linear theory GR f R0 =10-6 EJ, Baugh, Li, Zhao & Koyama 2012

CosmoSIS: modular cosmological parameter estimation Sarah Bridle, Scott Dodelson, Elise Jennings, Jim Kowalkowski, Alessandro Manzotti, Marc Paterno, Doug Rudd, Saba Sehrish, Joe Zuntz

Modular Calculations Zuntz et al 2014

CosmoSIS CosmoSIS Standard Library CAMB, Planck,WMAP, BICEP2,BOSS, CRL DES specific modules LSST specific modules CosmoSIS: -core libraries -infrastructure for modules to interact Software tools: gcc, g++, gfortran,python, SciPy, fftw, gsl,numpy, cfitsio, pyfits Other user s physics modules

Key highlights -easy download and install of all packages -access to 3rd party codes - CAMB, Planck, WMAP, CRL BICEP2 -End User can - contribute to CosmoSIS Standard Library - use other s code -get credit for their work -add modules in C, C++, fortran, Python -Provenance tracking https://bitbucket.org/joezuntz/cosmosis/wiki/home