• No se han encontrado resultados

The Formation History of the Ultra-Faint Dwarf Galaxies

N/A
N/A
Protected

Academic year: 2022

Share "The Formation History of the Ultra-Faint Dwarf Galaxies"

Copied!
50
0
0

Texto completo

(1)

The Formation History of the

Ultra-Faint Dwarf Galaxies

Tom Brown

Space Telescope Science Institute

(2)

Jason Tumlinson (STScI), Marla Geha (Yale), Evan N. Kirby (UC Irvine), Don A. VandenBerg (U of Victoria), Ricardo R. Munoz (U de Chile),

Jason S. Kalirai (STScI), Josh D. Simon (Carnegie),

Rorberto J. Avila (STScI), Puragra Guhathakurta (UCO/Lick), Alvio Renzini (INAF), Henry C. Ferguson (STScI),

Luis Vargas (Yale), Mario Gennaro (STScI)

The Formation History of the

Ultra-Faint Dwarf Galaxies

(3)

Overview

Background: ultra-faint dwarf galaxies

Hubble program overview

Ages in ultra-faint dwarfs

IMF in ultra-faint dwarfs

Summary

(4)

Tumlinson (2010)

Dark Matter Distribution

350 kpc

(5)

Tumlinson (2010)

Subhalos with star formation continuing past reionization

(6)

Tumlinson (2010)

Fossil subhalos - star formation truncated by reionization

(7)

Tumlinson (2010)

Most subhalos never form stars at all

(8)

SDSS Field of Streams

Belokurov et al. (2007)

(9)

Luminosity vs Size

1 10 100 1000

rh (pc) -2

-4 -6 -8 -10 -12 -14

M V (mag)

Globular Clusters

classical dSphs

ultra-faint dwarfs

Harris (1996) Mateo (1998) Martin et al. (2008)

(10)

Luminosity vs Size

Harris (1996) Mateo (1998) Martin et al. (2008)

1 10 100 1000

rh (pc) -2

-4 -6 -8 -10 -12 -14

M V (mag)

Globular Clusters

classical dSphs

ultra-faint dwarfs

(11)

Ground observations imply old populations in UFDs - but how old?

Leo IV (Sand et al. 2010)

MMT

Coma Berenices (Munoz et al. 2010)

CFHT

16

18

20

22

24

-0.5 0 0.5 1 1.5 2

I0

(V-I)0 UMa IUrsa Major I (Okamoto et al. 2008)

Subaru Bootes I

(Okamoto 2010) Subaru

Hercules (Sand et al. 2009)

LBT

Canes Venatici II (Greco et al. 2008)

WHT

0.0 0.5 1.0 1.5 B-V

(12)

Hubble Program Overview

Relative ages to <1 Gyr (SNR~100 at main sequence turnoff)

-

Relative to each other (synchronized star formation histories?)

-

Relative to ancient populations (e.g., globular clusters)

IMF in old dynamically un-evolved populations

Advanced Camera for Surveys (ACS) prime - centered on galaxy

Wide Field Camera 3 (WFC3) parallel - in galaxy outskirts

113 orbits - F606W (broad V) and F814W (I)

Comparison to ACS programs in the Local Group with same bands

-

Dozens of globular clusters (empirical ancient templates)

-

Many pencil-beam surveys of Local Group galaxies

Victoria-Regina Isochrones updated to latest physics

Leverage Keck spectroscopy to fix metallicities while fitting ages

(13)

Ursa Major I

ACS

WFC3

202’’ dist = 97 kpc

MV = -5.5 rh = 11.3’

rh = 318 pc 27 orbits

N E

(14)

Leo IV

ACS

WFC3

202’’

dist = 154 kpc MV = -5.8

rh = 4.6’

rh = 206 pc 16 orbits

N E

(15)

Leo IV 16 orbits faint limit

V~28.5

(16)

Leo IV 16 orbits faint limit

V~28.5

(17)
(18)

MSTO star V=24.8

MSTO star V=24.9

(19)

Leo IV 16 orbits faint limit

V~28.5

(20)
(21)

M92

(NGC 6341)

[Fe/H]=-2.3 (m-M)o=14.62

E(B-V)=0.023

(22)

M92

-1.2 -1.0 -0.8 -0.6 -0.4 -0.2 -0.0 0.2

m606 - m814 (STMAG) 24

22 20 18 16 14 12

m 814 (STMAG)

(23)

M92

-1.2 -1.0 -0.8 -0.6 -0.4 -0.2 -0.0 0.2

m606 - m814 (STMAG) 24

22 20 18 16 14 12

m 814 (STMAG)

"Empirical" Isochrone (Ridge Line)

Brown et al. (2005)

(24)

M92

-1.2 -1.0 -0.8 -0.6 -0.4 -0.2 -0.0 0.2

m606 - m814 (STMAG) 24

22 20 18 16 14 12

m 814 (STMAG)

Victoria-Regina Theoretical Isochrone Age = 13.0 Gyr [Fe/H]=-2.3

VandenBerg et al. (2012)

Notes:

[O/Fe] higher than assumed previously Teff-color relation empirically calibrated

(25)

Ages

(26)

-0.8 -0.6 -0.4 -0.2 0.0 m606-m814 (STMAG) 28

26 24 22 20 18

m 814 (STMAG)

Hercules

-0.8 -0.6 -0.4 -0.2 0.0 m606-m814 (STMAG) Leo IV

-0.8 -0.6 -0.4 -0.2 0.0 m606-m814 (STMAG) UMa I

28 26 24 22 20 18

m 814 (STMAG)

Boo I CVn II ComBer

Brown et al.

(2012, 2013 in prep)

(27)

-0.8 -0.6 -0.4 -0.2 0.0 m606-m814 (STMAG) 28

26 24 22 20 18

m 814 (STMAG)

Hercules M92

-0.8 -0.6 -0.4 -0.2 0.0 m606-m814 (STMAG)

Leo IV M92

-0.8 -0.6 -0.4 -0.2 0.0 m606-m814 (STMAG)

UMa I M92

28 26 24 22 20 18

m 814 (STMAG)

Boo I M92 CVn II M92 ComBer M92

Brown et al.

(2012, 2013 in prep)

(28)

-0.7 -0.6 -0.5 -0.4 -0.3 -0.2 -0.1 0.0 m606-m814 (STMAG)

29 28 27 26 25 24

m 814 (STMAG)

Hercules

CMDs of the UFDs, all look very similar

Composite UFD CMD looks like a single-age

population (to first order)

Brown et al. (2012, 2013 in prep)

(29)

CMDs of the UFDs, all look very similar

Composite UFD CMD looks like a single-age

population (to first order)

-0.7 -0.6 -0.5 -0.4 -0.3 -0.2 -0.1 0.0 m606-m814 (STMAG)

29 28 27 26 25 24

m 814 (STMAG)

Hercules Leo IV

Brown et al. (2012, 2013 in prep)

(30)

CMDs of the UFDs, all look very similar

Composite UFD CMD looks like a single-age

population (to first order)

-0.7 -0.6 -0.5 -0.4 -0.3 -0.2 -0.1 0.0 m606-m814 (STMAG)

29 28 27 26 25 24

m 814 (STMAG)

Hercules Leo IV CVn II

Brown et al. (2012, 2013 in prep)

(31)

CMDs of the UFDs, all look very similar

Composite UFD CMD looks like a single-age

population (to first order)

-0.7 -0.6 -0.5 -0.4 -0.3 -0.2 -0.1 0.0 m606-m814 (STMAG)

29 28 27 26 25 24

m 814 (STMAG)

Hercules Leo IV CVn II UMa I

Brown et al. (2012, 2013 in prep)

(32)

CMDs of the UFDs, all look very similar

Composite UFD CMD looks like a single-age

population (to first order)

Brown et al. (2012, 2013 in prep)

-0.7 -0.6 -0.5 -0.4 -0.3 -0.2 -0.1 0.0 m606-m814 (STMAG)

29 28 27 26 25 24

m 814 (STMAG)

Hercules Leo IV CVn II UMa I Boo I

(33)

Brown et al. (2012, 2013 in prep)

CMDs of the UFDs, all look very similar

Composite UFD CMD looks like a single-age

population (to first order)

-0.7 -0.6 -0.5 -0.4 -0.3 -0.2 -0.1 0.0 m606-m814 (STMAG)

29 28 27 26 25 24

m 814 (STMAG)

Hercules Leo IV CVn II UMa I Boo I Com Ber

(34)

-0.6 -0.5 -0.4 -0.3 m606-m814 (STMAG)

25.5 25.0 24.5 24.0

m 814 (STMAG)

Hercules

12.5 Gyr isochrone

-0.6 -0.5 -0.4 -0.3

m606-m814 (STMAG)

11.5 Gyr Model

12.5 Gyr isochrone

Brown et al.

(2012, 2013 in prep)

(35)

-0.6 -0.5 -0.4 -0.3 m606-m814 (STMAG)

25.5 25.0 24.5 24.0

m 814 (STMAG)

Hercules

12.5 Gyr isochrone

-0.6 -0.5 -0.4 -0.3

m606-m814 (STMAG)

12.5 Gyr Model

12.5 Gyr isochrone

Brown et al.

(2012, 2013 in prep)

(36)

-0.6 -0.5 -0.4 -0.3 m606-m814 (STMAG)

25.5 25.0 24.5 24.0

m 814 (STMAG)

Hercules

12.5 Gyr isochrone

-0.6 -0.5 -0.4 -0.3

m606-m814 (STMAG)

13.5 Gyr Model

12.5 Gyr isochrone

Brown et al.

(2012, 2013 in prep)

(37)

-0.6 -0.5 -0.4 -0.3 m606-m814 (STMAG)

25.5 25.0 24.5 24.0

m 814 (STMAG)

Hercules

12.5 Gyr isochrone

-0.6 -0.5 -0.4 -0.3

m606-m814 (STMAG)

12.5 Gyr Model

12.5 Gyr isochrone

Brown et al.

(2012, 2013 in prep)

(38)

Issues still being worked out

Distance & reddening to each UFD

-

Can affect age by ~0.5 Gyr

Field contamination in HST CMDs

-

Can mask trace sub-populations

Field contamination in Keck spectroscopy

-

Relatively metal-rich contaminants can drive a minority population that is ~1 to 2 Gyr younger in fit

[O/Fe] to assume in models at low [Fe/H]

-

Can affect age by ~0.5 Gyr

(39)

Initial Mass Function

(40)

Limited test in ideal population

Mass range is not large:

~0.5 - 0.8 MSun in 4: Hercules, Leo IV, UMa I, CVn II

~0.35 - 0.8 MSun in 2: Boo I & Com Ber

Old but dynamically un-evolved (unlike globular clusters)

IMF is a free parameter in many high-redshift studies

Test theoretical predictions IMF evolution

(e.g., Tumlinson 2010, Munoz et al. 2009, Bovill et al.

2009, Koposov et al. 2009, Li et al. 2010)

-

Larger characteristic mass at high z?

(due to higher CMB temperature)

(41)

24 25 26 27 28 m814 (STMAG)

10 100

number of stars

0.764 0.747 0.698 0.617 0.521 mass (MO .)

Hercules

25 26 27 28

m814 (STMAG) 10

100

0.766 0.755 0.716 0.643 0.548 mass (MO .)

Leo IV

Geha et al. (2013)

(42)

24 25 26 27 28 m814 (STMAG)

10 100

number of stars

0.764 0.747 0.698 0.617 0.521 mass (MO .)

Hercules

Best-fit power law (_=1.16)

25 26 27 28

m814 (STMAG) 10

100

0.766 0.755 0.716 0.643 0.548 mass (MO .)

Leo IV

Best-fit power law (_=1.31)

Geha et al. (2013)

(43)

24 25 26 27 28 m814 (STMAG)

10 100

number of stars

0.764 0.747 0.698 0.617 0.521 mass (MO .)

Hercules

Best-fit power law (_=1.16) Salpeter (1955; _=2.35)

25 26 27 28

m814 (STMAG) 10

100

0.766 0.755 0.716 0.643 0.548 mass (MO .)

Leo IV

Best-fit power law (_=1.31) Salpeter (1955; _=2.35)

Geha et al. (2013)

(44)

24 25 26 27 28 m814 (STMAG)

10 100

number of stars

0.764 0.747 0.698 0.617 0.521 mass (MO .)

Hercules

Best-fit power law (_=1.16) Salpeter (1955; _=2.35)

Bottom-light power law (_=0.5)

25 26 27 28

m814 (STMAG) 10

100

0.766 0.755 0.716 0.643 0.548 mass (MO .)

Leo IV

Best-fit power law (_=1.31) Salpeter (1955; _=2.35)

Bottom-light power law (_=0.5)

Geha et al. (2013)

(45)

Summary

Ultra-faint dwarf galaxies formed bulk (all?) of their stars 12 to 13 Gyr ago (z ~ 4 to 8)

No intermediate-age (< 10 Gyr) stars

-

Unlike most classical dwarf galaxies

Within current uncertainties, star formation is synchronized

-

Unclear if it predates reionization

IMF is flatter than Salpeter & other populations where directly measured (SMC, U Minor, MW)

(46)

Backup Slides

(47)

-4 -3 -2 -1 [Fe/H]

-1 0 1 2

[O/Fe]

Frebel (2009)

(48)

[O/Fe]

significantly

affects the age of the isochrone one would fit to a

color magnitude diagram

-0.7 -0.6 -0.5 -0.4 -0.3 -0.2

m606-m814 (STMAG) 8

6 4 2 0

m 814 (STMAG)

(49)

[O/Fe]

significantly

affects the age of the isochrone one would fit to a

color magnitude diagram

-0.7 -0.6 -0.5 -0.4 -0.3 -0.2

m606-m814 (STMAG) 8

6 4 2 0

m 814 (STMAG)

[Fe/H]=-2.35 [O/H]=-1.95 age=13.40 Gyr

(50)

[O/Fe]

significantly

affects the age of the isochrone one would fit to a

color magnitude diagram

-0.7 -0.6 -0.5 -0.4 -0.3 -0.2

m606-m814 (STMAG) 8

6 4 2 0

m 814 (STMAG)

[Fe/H]=-2.35 [O/H]=-1.95 age=13.40 Gyr

[Fe/H]=-2.35 [O/H]=-1.71 age=12.75 Gyr

Referencias

Documento similar

The circularized stellar mass density profiles for the galaxies in our sample, comparing them with similar mass SDSS ETGs and the massive compact galaxies in Szomoru et al..

• The Initial mass function and the nucleosynthesis stellar yields or production of new elements in stars, are two essential inputs for the chemical evolution

The simulated invariant mass spectrum was normalized to the data using the number of events in the mass interval 60–120 GeV.. The shape of this spectrum can be modified by

In the context of galaxy formation, two fundamental properties are given by the underlying dark matter structure: the distribution of their masses at a certain redshift as the halo

To do that, we have introduced, for both the case of trivial and non-trivial ’t Hooft non-abelian flux, the back- ground symmetric gauge: the gauge in which the stable SU (N )

By measuring the two-point correlation function of galaxy populations that differ in redshift, color, luminosity, star-formation history and bias, and using high-resolution

Ia, and also partially due to mas yields. Therefore, both IMF and massive stellar yields are playing a role here. It is evident that a ‘by eye’ inspection of these panels would

We introduce a toy model that describes (in a single equation) how much baryonic mass is accreted and retained into galaxies as a function of halo mass and redshift. In our model,