SLAC Summer Institute 2020 · 2020. 8. 11. · the cosmic microwave background. ... cosmological...

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Introduction to Cosmology II SLAC Summer Institute 2020 Daniel Gruen Panofsky Fellow, SLAC National Accelerator Laboratory August 11, 2020

Transcript of SLAC Summer Institute 2020 · 2020. 8. 11. · the cosmic microwave background. ... cosmological...

Page 1: SLAC Summer Institute 2020 · 2020. 8. 11. · the cosmic microwave background. ... cosmological model? 76. The contents of our Universe Based on all observations, ... 5% baryons

Introduction to Cosmology IISLAC Summer Institute 2020

Daniel GruenPanofsky Fellow, SLAC National Accelerator Laboratory

August 11, 2020

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Cosmic structure and Almost invisibles

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The Universe is homogeneous and isotropic.Wait a second....

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The Universe is homogeneous and isotropic,on sufficiently large scales

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Goals of today’s lecture● Understand structures in the Universe across

time, intuitively and with equations

● Understand the impact of almost invisibles on structures: neutrinos, dark matter, dark energy, even more hypothetical fields

● Get a sense of how we can measure the structure in the Universe, and what that has told us so far

● Set foundation for lectures this week

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Galaxy cluster MACS J0416, observed by the Dark Energy Survey

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The complete history of the Universe, as told by expansion

size ofUniversea(t)

age of Universe t 45

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The complete history of the Universe, as told by structure

size ofUniversea(t)

age of Universe t 46

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First: how do we quantify structure

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Dark Sky Simulation (Skillman+2014) Visualization: Ralf Koehler (SLAC)

density

density contrast

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First: how do we quantify structure - count of peaks

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density

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First: how do we quantify structure - full PDF

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First: how do we quantify structure - power spectrum

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The seeds of structure

● The early Universe’s vacuum hosted quantum fluctuations● These were expanded by inflation to cosmological scales● What happened to these fluctuations depended on their scale

relative to the horizon:○ While within the horizon, decay / stretched out by expansion○ When larger than horizon, preserved from decay

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almost invisible

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The seeds of structure

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almost invisible

● The early Universe’s vacuum hosted quantum fluctuations● These were expanded by inflation to cosmological scales● What happened to these fluctuations depended on their scale

relative to the horizon:○ While within the horizon, decay / stretched out by expansion○ When larger than horizon, preserved from decay

● For continuing inflation, this produces “scale invariant” power spectrum:

● But inflation has to end somehow

power

scale

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The seeds of structure

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almost invisible

● The early Universe’s vacuum hosted quantum fluctuations● These were expanded by inflation to cosmological scales● What happened to these fluctuations depended on their scale

relative to the horizon:○ While within the horizon, decay / stretched out by expansion○ When larger than horizon, preserved from decay

● For continuing inflation, this produces “scale invariant” power spectrum:

● But inflation has to end somehow: ns=1-ϵ

power

scale

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The seeds of structure also seed gravitational waves

● The early Universe’s vacuum hosted quantum fluctuations● These can include tensor perturbations to the metric

gravitational waves!

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almost invisible

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The seeds of structure also seed gravitational waves

● The early Universe’s vacuum hosted quantum fluctuations● These can include tensor perturbations to the metric

gravitational waves!

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almost invisible

Source: BICEP2

These could be detectable as B-mode polarization patterns of the cosmic microwave background

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The seeds of structure immersed in a hot Universe

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● Relativistic motion washes out density fluctuations at scales smaller than the horizon

● At the right scale, Baryons compress in matter overdensities right as the era of pressure ends

power

scaleHu & White 2004

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The seeds of structure immersed in a hot Universe

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● Relativistic motion washes out density fluctuations at scales smaller than the horizon

● At the right scale, Baryons compress in matter overdensities right as the era of pressure ends

● At half the scale, pressure counteracts the growth of fluctuations in the second half of the era of pressure

power

scale Hu & White 2004

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The seeds of structure immersed in a hot Universe

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● Relativistic motion washes out density fluctuations at scales smaller than the horizon

● At the right scale, Baryons compress in matter overdensities right as the era of pressure ends

● At half the scale, pressure counteracts the growth of fluctuations in the second half of the era of pressure

● This results in a characteristicpattern of temperature fluctuationpower spectrum: “BAO peak”

● Amplitude of temperature fluctuations: ~10-5

● Matter power spectrum now:power

scale Hu & White 2004Hu & White 2004

angu

lar p

ower

of

tem

pera

ture

fluc

tuat

ions

tiny to begin with heavily dampedfirst-peak scale

totally visible

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With BAO, you can measure distances

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Structure growth in the matter-dominated Universe

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𝜌’>𝜌

𝜌=𝜌crit

An overdense patch in a flat, matter-only Universe, same current expansion rate

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Structure growth in the matter-dominated Universe

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𝜌’

��expansion rate ofoverall Universe

overdense patch

𝜌=𝜌crit

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Structure growth in the matter-dominated Universe

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𝜌’

��

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Structure growth in the matter-dominated Universe

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● The amplitude of small density fluctuations grows as fast as the scale of the Universe!● The amplitude of small density fluctuations grows independent of their scale!

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Structure growth in the matter-dominated Universe

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● The amplitude of small density fluctuations grows as fast as the scale of the Universe!● The amplitude of small density fluctuations grows independent of their scale!

Wait a second:● Temperature fluctuations in the CMB at a=0.001 are δ~10-5

● By a=0.1, we have galaxies, which need δ or order 100● What did we miss?

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Structure growth in the matter-dominated Universe

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● The amplitude of small density fluctuations grows as fast as the scale of the Universe!● The amplitude of small density fluctuations grows independent of their size!

● This only produces any virialized structure when you account for○ The fact that pressureless dark matter already clusters during the radiation era○ The fact that once δ~1, this is a runaway process

almost invisible

Dark matter transfer

function

Growth factor,~a while matter dominates

Primordialpowerspectrum

+ non-linear terms on small scales

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An overdensity acts like a little universe of its own...

… but with higher matter density!

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Structure growth and Dark MatterThe null hypothesis is that Dark Matter is perfectly collisionless and cold.

What if Dark Matter was warm (like a Neutrino)?

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cold warm

simulated Milky Way-like dark matter distributionsBoehm+2014

almost invisible

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Structure growth and Dark MatterThe null hypothesis is that Dark Matter is perfectly collisionless and cold.

What if Dark Matter was self-interacting (like charged particles)?

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cold warm

simulated Milky Way-like dark matter distributionsBoehm+2014

hot gas

dark matterdark matter

almost invisible

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Structure growth and Dark Energy

● Dark Energy accelerates the expansion, even of mildly overdense patches, at late times

● That delays, or even stops, their collapse: growth is now less than proportional to a○ Measuring A2(z) constrains Dark Energy density and equation of state

● The unexpected presence of clusters at larger redshift was an early sign of Dark Energy existing

● Our local Supercluster will never form :(

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Laniakea supercluster

Perseus-Pisces superclusterTully+2014

almost invisible

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How to measure structure? Stay tuned!

size ofUniversea(t)

age of Universe t 75

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How to survey dark energy

Question:

Do all these measurements simultaneously agree with the same parameters of our cosmological model?

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The contents of our Universe

● Based on all observations, the universe is about 13.8 billion years old and today contains:

○ 70% vacuum energy

○ 25% dark matter

○ 5% baryons

● Time variations of dark energy equation of state are not well constrained

● Light new particles could influence early universe physics and expansion history

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Two tensions● Measurements of local expansion rate H0 disagree with the

parameter needed to describe expansion history at >4σ

○ Could point at additional particle(s) / interactions in early Universe that change size of “standard ruler”

○ Could point at very recent additional acceleration

○ Could point at systematic errors

● Measurement of late-time density fluctuation amplitudes disagree with early-time fluctuation amplitude at ~2-3σ

○ Could point at additional particle(s) / interactions

○ Could point at modifications of gravity

○ Could point at statistical fluke or systematic errors

Wong+2019 / Brout

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