Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University...

32
DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden

Transcript of Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University...

Page 1: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

DARK MATTER IN GALAXIESAlessandro Romeo

Onsala Space ObservatoryChalmers University of Technology

SE-43992 Onsala, Sweden

Page 2: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Overview

Dark matter in SPIRALS

Dark matter in ELLIPTICALS

Dark matter in DWARF SPHEROIDALS

Detecting dark matter

Conclusions

Page 3: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

SPIRALS

Page 4: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Stellar Discs

M33 very smooth structure

NGC 300 - exponential disc goes for at least 10 scale-lengths

Bland-Hawthorn et al 2005Ferguson et al 2003

scaleradius

Page 5: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

HI

Flattish radial distribution

Deficiency in the centre

CO and H2

Roughly exponential

Negligible mass

Wong & Blitz (2002)

Gas surface densities

GAS DISTRIBUTION

Page 6: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Early discovery from optical and HI RCs

MASS DISCREPANCY AT LARGE RADII

disk

observed

NO RC FOLLOWS THE DISK VELOCITY PROFILE

Rubin et al 1980

disk

Page 7: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

The mass discrepancy emerges as a disagreement between light and mass distributions

GALEX

SDSS

Extended HI kinematics traces dark matter

- -

NGC 5055 Light (SDSS) HI velocity field

Bosma, 1981

Bosma, 1981

Bosma 1979Radius (kpc)

Page 8: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Rotation Curves

Coadded from 3200 individual RCs

Salucci+07

6 RD

mag

TYPICAL INDIVIDUAL RCs OF INCREASING LUMINOSITY

Low lum

high lum

Page 9: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

The Concept of Universal Rotation Curve (URC)

The Cosmic Variance of the value of V(x,L) in galaxies of the same luminosity L at the same radius x=R/RD is negligible compared to the variations that V(x,L) shows as x and L vary.

The URC out to 6 RD is derived directly from observationsExtrapolation of URC out to virial radius by using

Page 10: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

A Universal Mass Distribution

ΛCDM URC Observed URC

NFW

high

low

Salucci+,2007

theory

obs

obs

Page 11: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Rotation curve analysisFrom data to mass models

➲ from I-band photometry

➲ from HI observations

➲ Dark halos with constant density cores (Burkert)

Dark halos with cusps (NFW, Einasto)

The mass model has 3 free parameters:

disk mass, halo central density and core radi radius (halo length-scale).

Vtot

2 = VDM

2 + Vdisk

2 + Vgas

2

NFW

Burkert

Page 12: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

core radius

halo central density

luminosity

disk

halo

halo

halo

diskdisk

MASS MODELLING RESULTS

fract

ion o

f D

M

lowest luminosities highest luminosities

All structural DM and LMparameters are related to luminosity.g

Smaller galaxies are denser and have a higher proportion of dark matter.

Page 13: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Dark Halo Scaling Laws

There exist relationships between halo structural quantiies and luminosity. Investigated via mass modelling of individual galaxies - Assumption: Maximun Disk, 30 objects-the slope of the halo rotation curve near the center gives the halo core density - extended RCs provide an estimate of halo core radius rc

Kormendy & Freeman (2004)

o ~ LB- 0.35

rc ~ LB 0.37

~ LB 0.20

o

rc

The central surface density ~ orc =constant 3.0

2.5

2.0

1.5

1.0

Page 14: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

SPIRALS: WHAT WE KNOW

A UNIVERSAL CURVE REPRESENTS ALL THE INDIVIDUAL RCsMORE PROPORTION OF DARK MATTER IN SMALLER SYSTEMSRADIUS AT WHICH THE DM SETS IN FUNCTION OF LUMINOSITYMASS PROFILE AT LARGER RADII COMPATIBLE WITH NFWDARK HALO DENSITY SHOWS A CENTRAL CORE OF SIZE 2 RD

Page 15: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

ELLIPTICALS

Page 16: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Surface brightness of ellipticals follows a Sersic (de Vaucouleurs) law

Re : the effective radius

By deprojecting I(R) we obtain the luminosity density j(r):

The Stellar Spheroid

R Rr

drrrjdzrjRI

22

)(2)()(

ESO 540 -032

Sersic profile

Page 17: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

SDSS early-type galaxies

The Fundamental Plane: central velocity dispersion, half-light radius and surface brightness are related

From virial theorem

FP “tilt” due to variations with σ0 of: Dark matter fraction? Stellar population?

Hyde & Bernardi 2009

Fitting

gives: a=1.8 , b~-0.8)then:

Bernardi et al. 2003

Page 18: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

RESULTSThe spheroid determines the velocity dispersionStars dominate inside R

e

More complications when:presence of anisotropiesdifferent halo profile (e.g. Burkert)

Two components: NFW halo, Sersic spheroid Assumed isotropy

Dark-Luminous mass decomposition of velocity dispersionsNot a unique model – example: a giant elliptical with reasonable parameters

Mamon & Łokas 05

Dark matter profile unresolved

1011

Page 19: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Weak and strong lensing

SLACS: Gavazzi et al. 2007)

Inside Re, the total (spheroid + dark halo) mass increases proportionally to the radius

Gavazzi et al 2007

UNCERTAIN DM DENSITY PROFILEI

Page 20: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Mass Profiles from X-ray

Temperature

Density

Hydrostatic Equilibrium

M/L profile

NO DM

Nigishita et al 2009

CORED HALOS?

Page 21: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

ELLIPTICALS: WHAT WE KNOW

A LINK AMONG THE STRUCTURAL PROPERTIES OF STELLAR SPHEROIDSMALL AMOUNT OF DM INSIDE RE

MASS PROFILE COMPATIBLE WITH NFW AND BURKERTDARK MATTER DIRECTLY TRACED OUT TO RVIR

Page 22: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

dSphs

Page 23: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Low-luminosity, gas-free satellites of Milky Way and M31

Large mass-to-light ratios (10 to 100 ), smallest stellar systems containing dark matter

Dwarf spheroidals: basic properties

Luminosities and sizes of Globular Clusters and dSph

Gilmore et al 2009

Page 24: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Velocity dispersion profiles

dSph dispersion profiles generally remain flat up to large radii

Wilkinson et al 2009

STELLAR SPHEROID

Page 25: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Mass profiles of dSphs

Jeans equation relates kinematics, light and underlying mass distribution

Make assumptions on the velocity anisotropy and then fit the dispersion profile

Results point to cored distributions

Jeans’ models provide the most objective sample comparison

Gilmore et al 2007

DENSITY PROFILE

n(R)

PLUMMER PROFILE

Page 26: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Degeneracy between DM mass profile and velocity anisotropyCusped and cored mass models fit dispersion profiles equally well

However: dSphs cored model structural parameters agree with those of Spirals and Ellipticals

Halo central density vs core radius

σ(R

) km

/s

Donato et al 2009

Walker et al 2009

NFW+anisotropy = CORED

Page 27: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

DSPH: WHAT WE KNOW

PROVE THE EXISTENCE OF DM HALOS OF 1010 MSUN AND ρ0 =10-21 g/cm3

DOMINATED BY DARK MATTER AT ANY RADIUS MASS PROFILE CONSISTENT WITH AN EXTRAPOLATION OF THE URC HINTS FOR THE PRESENCE OF A DENSITY CORE

Page 28: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

DETECTING DARK MATTER

Page 29: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.
Page 30: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

DM

Page 31: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

CONCLUSIONS

The distribution of DM halos around galaxies shows a striking and complex phenomenology.

Observations and experiments, coupled with theory and simulations, will (hopefully) soon allow us to understand two fundamental issues:

The nature of dark matter itself

The process of galaxy formation

Page 32: Dec. 1-8, 2010 DARK MATTER IN GALAXIES Alessandro Romeo Onsala Space Observatory Chalmers University of Technology SE-43992 Onsala, Sweden.

Thanks …..

That’s enough with Dark Matter!

Switch on the light ;-)

19.10.10