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Dark matter and strong lensing TOMMASO TREU (UCSB)

Dark matter and strong lensing

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Dark matter and strong lensing. TOMMASO TREU (UCSB). Outline. Introduction Cosmography Three key questions: Are dark matter halo profiles universal? (warm/ interactive dark matter?) Universal halos or universal stellar initial mass function? (a.k.a. non-baryonic dark matter?) - PowerPoint PPT Presentation

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Page 1: Dark matter and strong lensing

Dark matter and strong

lensingTOMMASO TREU (UCSB)

Page 2: Dark matter and strong lensing

Outline Introduction

Cosmography

Three key questions: Are dark matter halo profiles universal?

(warm/ interactive dark matter?) Universal halos or universal stellar

initial mass function? (a.k.a. non-baryonic dark matter?)

Is there dark matter substructure? (mass of the dark matter particle?)

Page 3: Dark matter and strong lensing

Strong gravitational Lensing

Image separation is a direct measurement of mass, luminous or dark!

Page 4: Dark matter and strong lensing

Why is it called Lensing?

Courtesy of P.J.Marshall

Page 5: Dark matter and strong lensing

Strong lensing is rare (1/1000 galaxy) but we know how to find lots of them

Page 6: Dark matter and strong lensing

Strong lensing in terms of Fermat’s principle

Excess time delay

Fermat distance

geometric time delay

Shapiro delay

Page 7: Dark matter and strong lensing

Cosmography

Page 8: Dark matter and strong lensing

H0 is needed for accurate measurements of

•Dark matter density•Flatness•Neutrino masses•Dark energy equation of state•…..

See Verde’s and Reid’s talk

Page 9: Dark matter and strong lensing

Cosmography from time delays:

how does it work?

Page 10: Dark matter and strong lensing

Cosmography with strong lenses:

4 solved problems Time delay – 2-3 %

Astrometry – 10-20 mas

Lens potential (2-3%)

Structure along the line of sight (2-3%)

Suyu et al. 2010

Page 11: Dark matter and strong lensing

Constraints for w=-1

Suyu et al. 2010

Page 12: Dark matter and strong lensing

Constraints on Dark Energy

For curved wCDM

With WMAP7:

• B1608+656 is comparable to BAO [Percival et al. 2010]

• B1608+656 and BAO both primarily constrain k

• SN [Hicken et al. 2009]

primarily constrains w

Page 13: Dark matter and strong lensing

Future Prospects

•Precision is 6-7% per system on H0 • Currently ~10 lenses have precise time-delays•Precision on H0 of <3% is attainable now•Future telescopes (e.g. LSST) will discover and measure 100s of time delays (Oguri & Marshall 2010; Treu 2010)

Page 14: Dark matter and strong lensing

Are dark matter profiles

universal? (warm/self

interacting dark

matter?)

Page 15: Dark matter and strong lensing

The mass density profile of dark matter halos

•Is the dark matter profile universal and “cuspy” as suggested by simulations?•If not, it may be a sign that dark matter is warm or self- interacting

De Blok’s talk

Page 16: Dark matter and strong lensing

Observational challenges…

•Precision over a large dynamic range in mass•Disentangle luminous and dark matter•Control systematics

Page 17: Dark matter and strong lensing

… can be overcome in clusters by combining

methods•Stellar kinematics (<30 kpc)•Strong lensing (<100 kpc)•X-ray (0.05 – 0.5 Mpc)•Weak lensing (0.1-3 Mpc)

Sand, Treu, Ellis 2002; Sand et al. 2004,2008; Newman et al. 2009,2011

Page 18: Dark matter and strong lensing

Newman et al 2011

Page 19: Dark matter and strong lensing

Results for Abell 611

Newman et al. 2009

Page 20: Dark matter and strong lensing

Results for Abell 383

Range of N-body resultsfor pure DM halo

Newman et al. 2011

More clusters on the way, see also Postman’s MCT

Page 21: Dark matter and strong lensing

The role of baryons

Baryonic cooling and star formation tends to drive material towards the center and thus make the inner slope steeper than for DM only

In simulations, the amount of steepening depends on the cluster merger history and the details of baryonic physics, because dynamical friction can counterbalance - at least in part - the effect

Page 22: Dark matter and strong lensing

Universal Halos or

Universal Stellar Initial

Mass function?

(Baryonic or non

baryonic?)

Page 23: Dark matter and strong lensing

Massive ellipticals have “too much” dark matter?

Treu et al. 2010

Stellar mass from lensing and dynamics

Ste

llar

mass f

rom

fro

m

colo

rs

Page 24: Dark matter and strong lensing

Universal halos or IMF?

Auger, TT et al. 2010

Salpeter

Kroupa

ChabrierIMF “

mis

matc

h”

Mass dependency

Page 25: Dark matter and strong lensing

What about spirals?

Dutton et al. 2011; Treu et al. 2011

Page 26: Dark matter and strong lensing

What about spirals?

Treu et al. 2011Dutton et al. 2011

Page 27: Dark matter and strong lensing

Is there dark matter

substructure?

(Mass of the dark

matter particle)

Page 28: Dark matter and strong lensing

Milky Way (missing) satellites

Kravtsov 2010 Strigari et al. 2007

Are they dark or do they not exist?

Page 29: Dark matter and strong lensing

“Missing satellites” and strong lensing

• Strong lensing detects satellites based on mass

• Satellites are detected as “anomalies” in the gravitational potential ψ

– ψ’’ = magnification anomalies

– ψ’ = astrometric anomalies

– ψ = time delay anomalies

Moustakas’ talk

Page 30: Dark matter and strong lensing

Gravitational mass imaging: idea

Mass substructure distorts extended lensed sources

Page 31: Dark matter and strong lensing

Direct detection of a dark substructure

Vegetti et al 2010

Page 32: Dark matter and strong lensing

Dark matter and strong lensing: Answers

Is there dark matter? What is it? Yes. We can help find out with time-delays

Are dark matter halo profiles universal? No. Either we do not understand baryons or

we do not understand dark matter

Is the IMF universal? No, If we understand dark matter halos.

Is there dark matter substructure? Yes. Not clear if there is enough (or maybe

too much)

Page 33: Dark matter and strong lensing

The end