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Galactic Winds in Dwarf Galaxies?

Galactic Winds in Dwarf Galaxies?

DGs

Dwarf as ideal Laboratories to study astrophysical Processes (a madley of research) Gerhard Hensler University of Vienna

Simone Recchi, Sylvia Ploeckinger, Lei Liu, Matthias Kuehtreiber, Patrick Steyrleithner, Bernhard Baumschlager, Thorsten Lisker

10/21/2018 and the SMAKCEDAmity team 6

Dwarf Galaxies as ideal Laboratories to study astrophysical Processes

 Morphological division of DGs  DG gas evacuation by galactic winds; Starbursts?  Transformation channel for dIrrs  dEs?  Starbursts by gas infall  dEs dominate in clusters: transformation by gas stripping  Self-regulated formation at low rates  DG formation from merger events? Tidal DGs!

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The Schematic View of DGs Smaller editions of Hubble-type galaxies? 6 10 10 -10 M, m 1-10 kpc, Mv>-18

Transformation paths from one morphological Sandage & Binggeli (1984) type to the other are proposed.

NGC 205 NGC 4214

M32 Antlia NGC 4449

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Correlations of different galaxy types

All “normal“ DGs, dEs and dIrrs follow the same relations even to their faintest end, but differ from UCDs+GCs and from the Hubble- type galaxies.

10/21/2018 Amity 9 Tolstoy et al. (2010) ARAA, 47

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Questions:

 Are Dwarf Galaxies as simple as they look like?

 Can one therefore understand their formation and evolution as simply?

 Did they have the same origin?

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Why are Dwarf Galaxies so interesting? They are extremely sensitive to 1) their formation epoch,

2) their internal evolution, 3) their environmental influence.

 different formation epochs  large variety of evolutionary paths  morphological transformations

DGs10/21/2018 are extremely Amityinteresting AP objects11

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DGs as building blocks in the hierarchical CDM scenario Dark Matter substructures form first and assemble to larger structures

but:

• Downsizing

• No clear DM content

10/21/2018 Amity • TDGs? 14

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Arp 188, the Tadpole Galaxy: bright knots as DG precursors?

bright star-formation knots are structured10/21/2018 within the tail. Amity 16

The Large Magellanic Clouds – a dIrr on its passage of the Milky Way: smooth evolution in interaction

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Starbursts + Galactic Wind Possible dIrr → dE transformation

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Possibility of dIrr  dE transition

DGs can show very active modes of , which can be triggered by environmental effects like e.g. gas infall or mergers.

Starburst can drive galactic winds! Can these winds evacuate dIrrs from their gas, i.e. transform them to dEs?

Understanding the cause of enhanced SF and the impact of massive on their environment is of fundamental relevance for  understanding the SF process,  galaxy evolution also in the Early Universe. 10/21/2018 Amity 19

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Dwarf Galaxies are strongly affected by Galactic Winds

In NGC 1569 2 Super Star Clusters at the base of the gas stream are the engines of the galactic wind due to their cumulative 10/21/2018 supernovaAmity II explosions. 20

Model: • bipolar outflow; • the S part towards observer is unobscured;  disk inclination known

• metal-enhanced wind: 1-2 Z!

X-ray in colors according to hardness (blue: hard, red: soft) overlaid with HI contours (white) 10/21/2018 Amity Martin et al. (2002) 21

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The mass loss can be determined from the effective yield yeff of the HI ISM. The loss of metals should be visible in the hot gas outflow.

Mass loading of super- bubbles diminishs their energetics (thermal+kinetic).

10/21/2018 Amity Martin et al. (2002)22 ApJ, 574

Metal loss through galactic outflows!

Garnett (2002)

Effective yields yeff of dIrrs < solar! Outflow of SNII gas reduces e.g. O. but: simple outflow models cannot account for gas mixing + turb. heating10/21/2018 Amity 23

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Galactic winds in Dwarf Galaxies?

Continuous mechanical L over 50 Myrs for various galaxy masses Mg and gas densities n: at t=50 Myrs

No consistent star formation!

10/21/2018 Amity 24 MacLow & Ferrara (1999)

t=100 Myrs

10/21/2018 Amity MacLow25 & Ferrara (1999)

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Galactic winds in DGs and the fate of metals

Luminosity (1038 erg s-1) 0,1 1 10

106 0,18 1 1 1 0,99 1

7

) 10 3.5e-3 8.4e-3 4.8e-2 

M 1 1 1

8

Mass ( 10 1.1e-4 3.4e-4 1.3e-3 0,8 1 1 Mass ejection efficiencies Metal ejection efficiencies

10/21/2018 Amity 27 MacLow & Ferrara (1999)

Can strong Galactic Winds solve the CDM cusp/core problem? Loss of low-ang.mom. gas!

(2010) Nature, 463 (2012) MNRAS, 422

NO 10solution/21/2018 when metal. mismatchAmity ! 28

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Testing galactic winds Starburst DGs and BCDGs remain gas-rich and are in different gas disks not exploding, but show perturbed gas dynamics.

Observed gas ouflows below escape velocities

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Recchi & Hensler (2013) A&A, 551 Testing galactic winds in different gas disks

Initial conditions:

7 8 9 • Baryonic mass: Mb = 10 , 10 , 10 M • Stellar disk by Myamoto-Nagai potential

• Isothermal gas disk with flattening b/a = 0.2, 1.0, 5.0 • Gas fraction: 60% (L), 90% (H)

• Spherical DM halo with MDM = 10 Mb • SFR~2

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Testing galactic winds in different gas disks

(2013) A&A, 551

SN ~ 5%

Blow-away of total gas almost impossible: Only in lowest-mass DGs and flat, light gas disks, but then all metals are lost. Gas disk, mixing, turbulence, external halo gas,10 /and21/2018 embedded clouds hamperAmity outflow . 31

Testing galactic winds in different gas disks

Oxygen ejection: Only lowest-mass DGs with lower gas fraction lose large O fractions. Thick gas disk and massive DGs retain their elements.

Recchi & Hensler (2013) A&A, 551

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Numerical Simulations of DG evolution Star-formation self-regulationby Stellar feedback 8 9 Mgas,i = 1.4 x10 M ; Ms,i = 0 Mgas,i = 2 x10 M ; Ms,i = 0 8 9 MDM = 8.4 x10 M MDM = 9.4 x10 M vrot = 30 km/s vrot = ~50 km/s SF as in Köppen, Theis, G.H. (1998, AA, 331) n 4 (c,Tc )  Cnc exp{Tc 10 K}

AMR code FLASH Steyrleithner et al. (2017) SPH code Kuehtreiber et al. (2017)

Low star-formation rate; No galactic wind! SF concentrated to the central part; Structures form; giant gas holes

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Star formation is self-regulated!

What triggers Starbursts?

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NGC 1569 Gas Infall confirmed! see Muehle et al. (2005) H

HI

Stil & Isreal (2002)

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Gas infall triggers Starburst The case od NGC 1569: 6 • HI clouds (each ~10 M) fall towards in from a disk • 2 huge super star clusters are formed. (2005, AJ, 130)

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NGC 4449 a triggered starburst

10/21/2018 Amity 39 (Hunter et al. 1995)

10/21/2018 Amity 40 II Zw 40 (van Zee et al. 1997)

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I Zw 18 - a “Youthful-looking Galaxy May Be an Adult” perturbed dIrr with gas infall?

(Östlin10/ 21&/ 2018Kunth 2000) Amity 41 (van Zee et al. 1997)

But: super is NGC 1705 not formed in the center !!

• Single SSC formed: 5 age  10 Myrs, Mvir  10 M 8 • SSC embedded in HI disk: MHI  10 M • X-ray maxima surrounded by H loops, representing tips of a superbubble, expanding vertically to the HI disk, but confined

X-ray contours H overlaid on HI H 10/21/2018 (HenslerAmity et al. 1998) 2 kpc 43 Meurer et al. (1998)

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How are dwarf elliptical galaxies formed?

 dIrrs do not lose their gas completely by galactic winds!

 Are all dEs formed morphologically separately?

 How much environmental effects?

 How would dIrrs without gas look like?

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dE Galaxies dominate in clusters

Sandage et al. (1984) Binggeli et al. (1987)

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X-ray Gas in Galaxy Clusters

7 TIGM  10 K -4 ... -3 -3 nIGM  10 cm ZIGM  0.2 ... 0.4 Z

The Virgo Cluster, a merging complex

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 The vol. density of dIrrs fraction in clusters is the same as in the field.  dEs dominate the morphology in clusters!

What makes dIrrs  dEs?

 Which process drives gas loss?

1. Galactic winds, gas expulsion 2. Tidal stripping 3. Ram-pressure stripping

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dEs in Virgo show a variety of shapes + properties that

seem10/ 21to/2018 correlate with the Amity 50 radial cluster distribution.

How to distinguish between cluster-born dEs vs. fallen-in, ram-pressure stripped, and harassed former dIrrs?

Infalling field dEs not to be discussed!

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Distribution of Virgo dE ages (all dEs; Hielscher, Janz et al.), with X-ray contours overplotted. red=older, slower blue=younger, faster

dEs as products of infalling RPS dIrrs are expected to • be at higher ICM densities • be at large cluster-centric distances, • to be flatter, • to have smaller Z, • move faster, eccentr. orbits 10/21/2018 Amity 52 Lisker, Janz, Hensler, et al. (2009) ApJ, 706

Dwarf Galaxies are expected to lose gas at cluster infall already by the low-density ICM ram pressure How much gas loss? Ram-pressure effects on star formation: In the DG body? In the RPS gas tail?

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Star formation in the RPS blobs The detection of -4 -3 with rates of ~ 10 … 10 M/yr ESO 137-001

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The case of VCC1217

Transformation by RPS

RGB UV,U,B,V

Hα-off

Hα-on not nec. SF!

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Gas Loss of DGs by strong RPS Mori & Burkert (2000)

10/21/2018 Amity 56 see also: Roediger & Hensler (2005)

Noeske et al. (2000) A&A, 361, 33

Transformation of dIrrs by RPS should be visible already in

a dilute environment, if vrel is sufficiently large. 10/21/2018 Amity 57 Consequences for their abundances? Star formation?

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Metal-Poor cometary BCDs

HST V image of SBS 1415+437. Guseva10/ 21et/2018 al. (2003, A&A 407, 105) Amity 58

RPS acts more efficiently for Dwarf Galaxies, even already at low densities in the outskirts of clusters

Thorsten Lisker, priv. comm.

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The complexity and variety of dEs in the Virgo Cluster

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Stellar content, MAss and Kinematics of Cluster Early-type Dwarfs (SMAKCED): project of dEs in Virgo Cl. http://www.smakced.net Urich, L., Lisker, T., Janz, J., et al. (HENSLER, G.): Young, metal-enriched cores in early-type dwarf galaxies in the Virgo cluster based on colour gradients, 2017, Astron. Astrophys., 606, A135

Sen, S., Peletier, R.F., Boselli, A., et al. (HENSLER, G.): Na and Ca abundances in dwarf elliptical galaxies, 2018, MNRAS, in press

Toloba, E., Guhathakurta, P., Boselli, A., et al. (HENSLER, G.): and structural Properties of Virgo Cluster Dwarf early-type Galaxies from the SMAKCED Project. III. Trends as a Function of projected Distance from the Cluster Center. 2015, ApJ., 799, 172

Toloba, E., Guhathakurta, P., Peletier, R.F., et al. (HENSLER, G.): Stellar Kinematics and structural Properties of Virgo Cluster Dwarf early-type Galaxies from the SMAKCED Project. II. The Survey and a systematic Analysis of kinematic Anomalies and Asymmetries.. 2014, ApJ. Suppl., 215, 17

Janz, J., Laurikainen,, E.,Lisker, T., et al. (HENSLER, G.): A Near- Census of the Multi-Component of Early-Type Dwarf Galaxies in the Virgo Cluster . 2014, ApJ, 786, 105

Toloba, E., Guhathakurta, P., van de Ven, G., et al. (HENSLER, G.): Stellar Kinematics and Structural Properties of Virgo Cluster Dwarf Early-Type Galaxies from the SMAKCED Project. I. Kinematically Decoupled Cores and Implications for Infallen Groups in Clusters . 2014, ApJ, 783, 120

Janz, J. LaurikainenSS 2017 , E. Lisker, T., et al. (HENSLER, G.): Dissecting early-type dwarf galaxies into their multiple components . 2012, ApJL, 745, L24 61

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Modelling RPS DGs

8 Mgas,i = 1.4 x10 M ; Ms,i = 0 8 MDM = 8.4 x10 M vrot = 30 km/s -4 -3 vrel = 290 km/s, nICM = 10 cm

No enhanced SF No total gas evacuation

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RPS for very low-mass DGs

6 Mgas,i = 6.3 x10 M ; Ms,i = 0 . SF enhanced when vrel reaches max. 8 MDM = 1.2 x10 M . No SF in RPS gas tails vrot = 2 km/s . Gas almost totally lost, but moderate infall: vrel = 290 km/s, condensed clouds survive with -4 -3 nICM = 10 cm varying SFRs

Steyrleithner et al., 2018, in prep.

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fast RPS DGs

6 Mgas,i = 6.3 x10 M ; Ms,i = 0 8 MDM = 1.2 x10 M vrot = 2 km/s fast infall: vrel = 1000 km/s, -4 -3 nICM = 10 cm

Steyrleithner et al. in prep.

. Critical velocity for enhanced SF is reached earlier not when

vrel max. . Gas almost totally lost, but condensed clouds survive . When these condensed clumps

10/21/2018 Amity get RP stipped at later stages,64 they bear SF

Galaxy Cluster DGs:

DGs are RP stripped in low-density inter-galactic medium!

Star formation enhanced due to ram pressure!

SF in stripped clumps: Under which conditions? Where observable? Steyrleithner et al. (GH) 2018, MN, to be submitted

Gas loss + harassment! Smith et al. (GH) 2015, MN

How do transformed dEs look like? See SMAKCED publ.s 10/21/2018 Amity 65

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Virgo dEs with kinematically decoupled cores

VCC 1183

So far only known in Es and caused by gas/galaxy !

Yet no plausible explanation for dEs!

Toloba et al. (GH), 2014, ApJ, 783

( Amity 66

The KDCs of VCC1183 and VCC1453 are younger than the main body. Unsolved problem of the KDC formation: …… SS 2017 67

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7. Star-formation history in Virgo dEs

Koleva et al. 2009, MNRAS, 396

SS 2017 68

Summing up Dwarf Galaxies:  DGs‘ evolution is highly complex! Gas outflows and infall, transformation  DGs morphology results from their environment! Starbursts by gas infall vs. numerical tricks? As satellites of mature galaxies!  Morphological transformations are possible: Cluster dEs of different origin; cl.-born vs. infall!  Starbursts by gas accretion (or stochastically?)  DGs as probes of astrophysical processes and numerical prescriptions: star-formation recipes, ISM phases  TDGs are a potential reservoir of replacing destroyed DGs. DGs10/21/ 2018are challenging CDM cosmologyAmity 69

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THANK YOU

for your attention !!! - Glad to be here and to seeing you for discussions and collaborations

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Summing up Dwarf Galaxies:  DGs‘ evolution is highly complex! Gas outflows and infall, transformation  DGs are results of their environment! Cluster dEs of different origin! Starbursts by gas accretion (or stochastically?)  DGs‘ CDM formation questionable: Continues production-transformation-mass loss/accretion cycle?  TDGs survive without DM: DG fraction?  What does their distribution in the local Universe teach us? More observational and modelling details requested!  Present-day gas accumulation:

HI10/21-/2018dominated LSB DGs Amity 71

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