Cosmology in the Time of Dark Energy Lecture

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Cosmology in the Time of Dark Energy Lecture 1 Ignacy Sawicki CEICO, Institute of

Cosmology in the Time of Dark Energy Lecture 1 Ignacy Sawicki CEICO, Institute of Physics, CAS, Prague ceico

Rough Outline � Main assumptions in cosmology � Acceleration: how robust? � What can

Rough Outline � Main assumptions in cosmology � Acceleration: how robust? � What can we know without GR? � Main aim: lay out the logic/assumptions behind what we do 20 July 2018 4 th Cosmology School, UJ

Expt. Physics vs 20 July 2018 4 th Cosmology School, UJ Cosmology

Expt. Physics vs 20 July 2018 4 th Cosmology School, UJ Cosmology

Making Sense of the Sky � 20 July 2018 4 th Cosmology School, UJ

Making Sense of the Sky � 20 July 2018 4 th Cosmology School, UJ

Making Sense of the Sky 20 July 2018 4 th Cosmology School, UJ

Making Sense of the Sky 20 July 2018 4 th Cosmology School, UJ

Making Sense of the Sky Redshift 20 July 2018 4 th Cosmology School, UJ

Making Sense of the Sky Redshift 20 July 2018 4 th Cosmology School, UJ

Ordering by redshift 20 July 2018 4 th Cosmology School, UJ Image credit: Ivo

Ordering by redshift 20 July 2018 4 th Cosmology School, UJ Image credit: Ivo Labbé

Use Standard Candles to Map 20 July 2018 4 th Cosmology School, UJ

Use Standard Candles to Map 20 July 2018 4 th Cosmology School, UJ

SN Ia: Universal Objects Image credit: D. Butler 20 July 2018 4 th Cosmology

SN Ia: Universal Objects Image credit: D. Butler 20 July 2018 4 th Cosmology School, UJ

Use Standard Candles to Map 20 July 2018 4 th Cosmology School, UJ

Use Standard Candles to Map 20 July 2018 4 th Cosmology School, UJ

First Attempt at a Model � The Copernican Principle: here is not special Isotropy

First Attempt at a Model � The Copernican Principle: here is not special Isotropy 20 July 2018 Homogeneity 4 th Cosmology School, UJ

First Attempt at a Model � The Copernican Principle: here is not special Isotropy

First Attempt at a Model � The Copernican Principle: here is not special Isotropy Homogeneity Planck (2015) 20 July 2018 Wiggle. Z: Scrimgeur et al. (2012) 4 th Cosmology School, UJ

First Attempt at a Model � Hubble parameter 20 July 2018 4 th Cosmology

First Attempt at a Model � Hubble parameter 20 July 2018 4 th Cosmology School, UJ

First Attempt at a Model 2. Composition: slowly-moving or virialised objects Late universe comprises

First Attempt at a Model 2. Composition: slowly-moving or virialised objects Late universe comprises mostly nonrelativistic matter sources (dust) 20 July 2018 4 th Cosmology School, UJ

First Attempt at a Model 3. Theory of gravity: General Relativity Monica Witt 20

First Attempt at a Model 3. Theory of gravity: General Relativity Monica Witt 20 July 2018 4 th Cosmology School, UJ

From D. Huterer Dimmer First Attempt at Model: FAIL 20 July 2018 4 th

From D. Huterer Dimmer First Attempt at Model: FAIL 20 July 2018 4 th Cosmology School, UJ

Conservation of Energy � 20 July 2018 4 th Cosmology School, UJ

Conservation of Energy � 20 July 2018 4 th Cosmology School, UJ

How to increase distances? � 20 July 2018 4 th Cosmology School, UJ

How to increase distances? � 20 July 2018 4 th Cosmology School, UJ

Planck 2018 COMPOSITION OF UNIVERSE IF ΛCDM Dark Matter 26% Cosmological Constant 69% Baryons

Planck 2018 COMPOSITION OF UNIVERSE IF ΛCDM Dark Matter 26% Cosmological Constant 69% Baryons 5% (stars 0. 4%, gas 4. 6%) 20 July 2018 4 th Cosmology School, UJ

Is the Universe fooling us? � 20 July 2018 4 th Cosmology School, UJ

Is the Universe fooling us? � 20 July 2018 4 th Cosmology School, UJ

The FLRW Lightcone 20 July 2018 4 th Cosmology School, UJ

The FLRW Lightcone 20 July 2018 4 th Cosmology School, UJ

The inhomogeneous alternative � 20 July 2018 4 th Cosmology School, UJ

The inhomogeneous alternative � 20 July 2018 4 th Cosmology School, UJ

Is the Universe fooling us? Acceleration detected at 64σ 20 July 2018 4 th

Is the Universe fooling us? Acceleration detected at 64σ 20 July 2018 4 th Cosmology School, UJ

Summary 1: Acceleration � Distances purely cosmography: � Need EM and metric � No

Summary 1: Acceleration � Distances purely cosmography: � Need EM and metric � No theory of gravity � Assumption 1: sources do not evolve in time � Copernican principle: we are not in a special place � This is enough to show there is acceleration � To predict/interpret need to models � Composition: late universe is made of slowly moving stuff � Theory of gravity to link stuff to metric 20 July 2018 4 th Cosmology School, UJ

So, what is it? 20 July 2018 4 th Cosmology School, UJ

So, what is it? 20 July 2018 4 th Cosmology School, UJ

The cosmological constant � 20 July 2018 4 th Cosmology School, UJ

The cosmological constant � 20 July 2018 4 th Cosmology School, UJ

The cosmological constant e. g. Jerome Martin (2012) � 20 July 2018 4 th

The cosmological constant e. g. Jerome Martin (2012) � 20 July 2018 4 th Cosmology School, UJ

Maybe it’s not stuff, but gravity? Baker, Psaltis, Skordis (2015) Binary PSR Solar System

Maybe it’s not stuff, but gravity? Baker, Psaltis, Skordis (2015) Binary PSR Solar System 20 July 2018 4 th Cosmology School, UJ

Tenets of Modifying Gravity � Accept Copernican Principle: universe is FRW with small fluctuations

Tenets of Modifying Gravity � Accept Copernican Principle: universe is FRW with small fluctuations � Let go of Einstein equations: replace them with what? � Accept standard inflationary initial conditions: why is this here? 20 July 2018 4 th Cosmology School, UJ

Initial Conditions vs Transfer Fns Einstein + Boltzmann eqs Verde & Peiris (2008) Planck

Initial Conditions vs Transfer Fns Einstein + Boltzmann eqs Verde & Peiris (2008) Planck (2015) Einstein + Boltzmann eqs 20 July 2018 4 th Cosmology School, UJ Pratten (2016)

Tenets of Modifying Gravity � Accept Copernican Principle: universe is FRW with small fluctuations

Tenets of Modifying Gravity � Accept Copernican Principle: universe is FRW with small fluctuations � Let go of Einstein equations: replace them with what? � Accept standard inflationary initial conditions: why is this here? 20 July 2018 4 th Cosmology School, UJ

Modify Friedmann Eq � This is not a model… 20 July 2018 4 th

Modify Friedmann Eq � This is not a model… 20 July 2018 4 th Cosmology School, UJ

Measure Distances: Cosmography Supernovae Image: HSR Baryon Acoustic Oscillations Image: Z. Rostomian, LBNL 20

Measure Distances: Cosmography Supernovae Image: HSR Baryon Acoustic Oscillations Image: Z. Rostomian, LBNL 20 July 2018 4 th Cosmology School, UJ

So we constrain the Eo. S. Or? Planck: Ade et al. (2013) Planck +

So we constrain the Eo. S. Or? Planck: Ade et al. (2013) Planck + WP w Planck + WP + BAO 20 July 2018 4 th Cosmology School, UJ

But w is not an observable � 20 July 2018 4 th Cosmology School,

But w is not an observable � 20 July 2018 4 th Cosmology School, UJ Kunz (2007)

Andrew Liddle 20 July 2018 4 th Cosmology School, UJ

Andrew Liddle 20 July 2018 4 th Cosmology School, UJ

Andrew Liddle Dark Matter 20 July 2018 Dark Energy 4 th Cosmology School, UJ

Andrew Liddle Dark Matter 20 July 2018 Dark Energy 4 th Cosmology School, UJ

Andrew Liddle 20 July 2018 Dark Matter Dark Energy Clusters Unclustered 4 th Cosmology

Andrew Liddle 20 July 2018 Dark Matter Dark Energy Clusters Unclustered 4 th Cosmology School, UJ

Andrew Liddle 20 July 2018 Dark Matter Dark Energy Clusters Clustering 4 th Cosmology

Andrew Liddle 20 July 2018 Dark Matter Dark Energy Clusters Clustering 4 th Cosmology School, UJ

Distances consistent with ΛCDM Zhao et al. (2018) BOSS DR 14 20 July 2018

Distances consistent with ΛCDM Zhao et al. (2018) BOSS DR 14 20 July 2018 4 th Cosmology School, UJ

Distances consistent with ΛCDM Planck (2018) 20 July 2018 4 th Cosmology School, UJ

Distances consistent with ΛCDM Planck (2018) 20 July 2018 4 th Cosmology School, UJ

Measuring the Hubble rate today W. Freedman 20 July 2018 4 th Cosmology School,

Measuring the Hubble rate today W. Freedman 20 July 2018 4 th Cosmology School, UJ

H 0 is not observable � 1 --5 December 2014 X Mexican School on

H 0 is not observable � 1 --5 December 2014 X Mexican School on Gravitation Marra et al. (2013)

Summary 2: c. c. and background � 20 July 2018 4 th Cosmology School,

Summary 2: c. c. and background � 20 July 2018 4 th Cosmology School, UJ