Cosmology from Space

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Cosmology from Space Max Tegmark, MIT

description

Cosmology from Space. Max Tegmark, MIT. Smorgasbord. Hinshaw, Wandelt. Galaxy surveys. Microwave background. Supernovae Ia. THE COSMIC SM Ö RG Å SBORD. Gravitational lensing. Big Bang nucleosynthesis. Abazajian. Galaxy clusters. Neutral hydrogen tomography. Lyman  forest. - PowerPoint PPT Presentation

Transcript of Cosmology from Space

Page 1: Cosmology from Space

Cosmology from Space

Max Tegmark, MITMax Tegmark, MIT

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Smorgasbord THE COSMIC

SMÖRGÅSBORD

Galaxy surveys

Microwave background

Gravitational lensing

Big Bang nucleosynthesis

Supernovae Ia

Galaxy clusters

Lyman forest

Neutral hydrogen tomography

Hinshaw,Wandelt

Abazajian

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What have we learned?

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

OUR PLACE IN SPACE

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DSE

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

OUR PLACE IN TIME

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Fluctuation generator

Fluctuation amplifier

(Graphics from Gary Hinshaw/WMAP team)

Hot Dense SmoothCool Rarefied

Clumpy

Brief History of our Universe

400

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Formation movies

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EVIDENCE?

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Riess et al, astro-ph/0611572

What we’ve learned about the cosmic expansion history from SN Ia

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008Nolta et al 2008, arXiv:0803.0593

2008:

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Max TegmarkDept. of Physics, MIT

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July 7, 2008

Cmbgg OmOl

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Cmbgg OmOl

Ordinary Matter5%

Dark Energy72%

Cold Dark Matter23%

Ordinary Matter

Dark Energy

Cold Dark Matter

Hot Dark Matter

Photons

Budget Deficit

4% 21%

75%Using WMAP3 + SDSS LRGs:

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Cmbgg OmOl

430

386

13.8

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Cosmological data

Cosmological Parameters

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Cosmological data

Cosmological Parameters

ARE WE DONE?

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

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4%

75%

21%

Cosmological data

Fundamental theory ?

Cosmological Parameters

Nature of dark matter?

Nature of dark energy?

Nature of early Universe?

Why these particular values?

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Four roads to dark matter: catch it, infer it, make it, weigh it

Direct:

Indirect:

Production:

GLAST launched 6/11-08

Gravitational:

Planck launch scheduled for December 2008

21 cm tomography coming

Dermer,Kusenko, …

Wandelt

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4%

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Cosmological data

Fundamental theory ?

Cosmological Parameters

Nature of dark matter?

Nature of dark energy?

Nature of early Universe?

Why these particular values?

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How did it all begin?

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Herman, Gamow & Alpher, 1940’s

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Arno Penzias & Robert Wilson 1965

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100dpi

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

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?

(Graphics fromWMAP team)

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History

(Figure from Wayne Hu)

(Figure from WMAP team)

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History

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

History

CMBF

oreg

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d-cl

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d W

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, de

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History

Q: How see through this wall?

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History

Q: How see through this wall?

A: With gravitational waves!

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Max TegmarkDept. of Physics, MIT

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Cmbgg OmOl

CMB

+

LSS

(Figure from Matias Zaldarriaga)

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SN Ia+CMB+LSS constraintsYun Wang & MT, PRL 92, 241302

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tot

, w

Q, ns, , r, nt

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CMB polarization missions

Dark Energy missions

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Why should you believe this?

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Max TegmarkDept. of Physics, MIT

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July 7, 2008

Boomzoom

Gut

h &

Kai

ser

2005

, Sci

ence

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Max TegmarkDept. of Physics, MIT

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July 7, 2008

Cmbgg OmOl

How flat is space?

flat

closedopen

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Max TegmarkDept. of Physics, MIT

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July 7, 2008

Cmbgg OmOl

How flat is space?

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Cmbgg OmOl

How flat is space? Somewhat.

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Cmbgg OmOl

tot=1.003How flat is space?

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Cmbgg OmOl

CMB

+

LSS

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Cmbgg OmOl

CMB

+

LSS

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Cmbgg OmOl

CMB

+

LSS

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Cmbgg OmOl

CMB

+

LSS

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Cmbgg OmOl

CMB

+

LSS

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Cmbgg OmOl

CMB

+

LSS

CMB polarization + SDSS: n=0.008, r=0.01

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Page 54: Cosmology from Space

Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

SKEPTIC: COUNTER:

Won’t find anything, 1: Inflation energy could be anywhere from 103 to 1016 GeV, so very unlikely that ~1016 and hence detectable.

This ignores that we’ve measured Q~10-5. Either we had classic (slow-rolling scalar field) inflation, in case we’ll see it, or we didn’t, and all bets are off. Also, GUT scale natural candidate for new physics.

Won’t find anything, 2: There are theoretical arguments against high energy inflation (hard for to roll many Planck units).

There are are counterexamples, like N-flation. Moreover, there are theoretical arguments against low energy inflation (landscape ns problem).

Will be killed by foregrounds and systematics.

These are very serious challenges, but detailed studies suggest that they can be overcome, just as they have so far. Going to space helps enormously!

Very focused mission (as opposed to serving broader astrophysical community)

CMB maps have proven useful for research on Galactic structure, ISM, Galactic B-field, cluster SZ effect, etc.

Technology not ready Far along, can be ready on time as long as ball not dropped (see Weiss report)

So is CMBpol satellite worthwhile?

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4%

75%

21%

Cosmological data

Fundamental theory ?

Cosmological Parameters

Nature of dark matter?

Nature of dark energy?

Nature of early Universe?

Why these particular values?

Map our universe!

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Physics with neutral

hydrogen tomography

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

History

CMB

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Our observable universe

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LSS

Our observable universe

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LSS

The time frontier

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Cmbgg OmOl

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Max TegmarkDept. of Physics, MIT

[email protected] to Cosmos

July 7, 2008

Cmbgg OmOl

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Max TegmarkDept. of Physics, MIT

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LSS The scale frontier

(A. Klypin)(Q. Shafi)

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Max TegmarkDept. of Physics, MIT

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July 7, 2008 Tegmark & Zaldarriaga 2008

The sensitivity frontier

FFTT

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LSS

Our observable universe

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LSS

Our observable universe

Mao, MT, McQuinn, Zahn & Zaldarriaga 2008

Spatial curvature:WMAP+SDSS: tot= 0.01 Planck: tot= 0.00321cm: tot=0.0002

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LSS

Our observable universe

Spectral index running:Planck: =0.00521cm =0.000172-potential: 0.00074-potential: 0.008

Mao, MT, McQuinn, Zahn & Zaldarriaga 2008

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LSS

Our observable universe

Mao, MT, McQuinn, Zahn & Zaldarriaga 2008

Neutrino mass:WMAP+SDSS: m <0.3 eV+LyF: m <0.17 eV Oscillations m>0.04 eVFuture lensing: m~0.03 eV21cm: m=0.007 eV

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Boomzoom

1. No ionosphere

2. Shielding from terrestial radio noise

Advantages of deploying radio array here:

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Boomzoom

Participants: MIT, Harvard, Washington, Berkeley, JPL, NRAO

PI: Jacqueline Hewitt, MIT

LARC: Lunar Array for Radio Cosmology

Also DALI (Joe Lazio et al)

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