Gas content and gas kinema/cs in low-mass galaxies Leslie Hunt - - PowerPoint PPT Presentation

gas content and gas kinema cs in low mass galaxies
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Gas content and gas kinema/cs in low-mass galaxies Leslie Hunt - - PowerPoint PPT Presentation

Gas content and gas kinema/cs in low-mass galaxies Leslie Hunt INAF-Osservatorio Astrofisico di Arcetri, Firenze why low-mass (metal-poor) galaxies? UV luminosity func/onsz~4, z~8 low mass galaxies are the most Bouwens+ 2011 numerous at


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Gas content and gas kinema/cs in low-mass galaxies

Leslie Hunt INAF-Osservatorio Astrofisico di Arcetri, Firenze

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why low-mass (metal-poor) galaxies?

low mass galaxies are the most numerous at all redshiGs, very low-luminosity galaxies provide the dominant contribu/on to the luminosity density at z>6

(e.g., Bouwens+ 2011, 2012; Atek+ 2015; Sun & FurlaneUo 2016)

although dark-maUer haloes are built boUom-up, massive galaxies form their stars early

  • n (downsizing), unlike low-

mass galaxies that form a large frac/on of their stars later

Galaxy Stellar Mass func/ons to z~4 from Ilbert+ 2013, data from z~0 Moustakas+ 2013, Baldry+ 2012) UV luminosity func/onsz~4, z~8 Bouwens+ 2011 Specific star forma/on rate as func/on of look- back /me for galaxies of varying masses (Thomas+ 2010)

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SLIDE 3
  • utline of talk

INEFFICIENCY of star forma/on/galaxy mass assembly and the role of FEEDBACK feedback and gas/SFR scaling rela/ons (KennicuU-Schmidt) scaling rela/ons for low-mass galaxies: gas frac/ons, mass, SFR, metallicity (take note of metal-poor starbursts) feedback and the baryonic Tully-Fisher rela/on: contribu/on of molecular gas in low-mass (metal-poor) starbursts pressure support and turbulence, comparison of different tracers in low-mass galaxies Low-mass galaxies important probe of galaxy forma/on scenarios because of their vulnerability to feedback

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feedback and the inefficiency of galaxy mass assembly and star forma/on

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SLIDE 5

stellar and baryon frac/on in dark-maUer halos

stellar mass depends on dark-maUer halo mass, but rela/vely independent of redshiG (lookback /me)

Behroozi+ 2013a, 2013b (see also Moster+ 2013, Genel+ 2014) star-forma/on efficiency (SFE) peaks at 5x1011 M¤, characteris/c mass “sweet spot” for galaxy forma/on z=0

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feedback renders galaxy forma/on inefficient

Hopkins+ 2014, FIRE simula/ons Stellar mass (M¤) Halo mass (M¤) Stellar /baryonic “sweet spot” at 5x1011 M¤ Stellar /baryonic Stellar /baryonic Halo mass (M¤)

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SLIDE 7

Stellar /baryonic Stellar /baryonic Halo mass (M¤)

feedback renders galaxy forma/on inefficient

models without feedback are in severe conflict with observa/ons, especially at low masses Stellar mass (M¤) Halo mass (M¤) Stellar /Baryonic “sweet spot” at 5x1011 M¤ Hopkins+ 2014, FIRE simula/ons

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SLIDE 8

feedback and gas scaling rela/ons

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SLIDE 9

star forma/on is inefficient because of feedback

Hopkins+ 2014 KennicuU-Schmidt (KS) law rela/ng SFR and gas surface densi/es; observa/ons (KennicuU 1998; Bigiel+ 2008; Genzel+ 2010; Daddi + 2010) indicated by yellow shaded region. Simula/ons including various recipes for feedback (see previous slide) shown by points. Instantaneous SFE (here SF per dynamical /me) in dense gas is 100%, but global SFE is ~2%.

stellar feedback injects sufficient momentum to offset dissipa/on; otherwise too- efficient cooling would cause all gas to collapse and form stars

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SLIDE 10

inefficient star forma/on in metal-poor galaxies?

lower intercepts for lines (with unit slope) in this plane mean longer gas deple/on /mes starbursts and high-z galaxies tend to have shorter gas deple/on /mescales (here αCO converted to common scale, e.g., Genzel, Tacconi+ 2010)

100 101 102 103 104 10−4 10−3 10−2 10−1 100 101 102 103 Σgas [Msun pc−2] ΣSFR [Msun yr−1 kpc−2]

10Gyr 1Gyr 100Myr SMGs Genzel+ (2010) SFGs Tacconi+ (2010, 2013) BzKs Daddi+ (2010) Spirals Kennicutt (1998) Starbursts Kennicutt (1998)

All resolved measurements (except Kennicutt)

False colors: Bigiel+ (2008)

K r u m h

  • l

z + ( 2 9 )

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SLIDE 11

100 101 102 103 104 10−4 10−3 10−2 10−1 100 101 102 103 Σgas [Msun pc−2] ΣSFR [Msun yr−1 kpc−2]

10Gyr 1Gyr 100Myr

  • ●●
  • SMGs Genzel+ (2010)

SFGs Tacconi+ (2010, 2013) BzKs Daddi+ (2010) Spirals Kennicutt (1998) Starbursts Kennicutt (1998)

All resolved measurements (except Kennicutt)

  • Blue compact dwarfs (HI only)

LITTLE THINGS (HI only) SHIELD dwarfs (HI only) FIGGS dwarfs (HI only) VLA−ANGST dwarfs (HI only)

inefficient star forma/on in metal-poor galaxies?

Hunt+ in prep high ΣSFR and high ΣHI common in blue compact dwarf galaxies (BCDs), and some LiUle THINGS dwarfs, despite their low metallicity dwarfs may not all be inefficient at forming stars compare with high-redshiG popula/ons to consider the best local analogs

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inefficient star forma/on in metal-poor galaxies?

Hunt+ in prep 100 101 102 103 104 10−4 10−3 10−2 10−1 100 101 102 103 Σgas [Msun pc−2] ΣSFR [Msun yr−1 kpc−2]

10Gyr 1Gyr 100Myr

  • ●●
  • IIZw40

NGC1140

  • NGC5253

SBS0035−052 DDO87 NGC1569 IC10

SMGs Genzel+ (2010) SFGs Tacconi+ (2010, 2013) BzKs Daddi+ (2010) Spirals Kennicutt (1998) Starbursts Kennicutt (1998)

All resolved measurements (except Kennicutt)

  • Blue compact dwarfs (HI only)

LITTLE THINGS (HI only) SHIELD dwarfs (HI only) FIGGS dwarfs (HI only) VLA−ANGST dwarfs (HI only)

Ruby (Canameras+ 2017) high ΣSFR and high ΣHI common in blue compact dwarf galaxies (BCDs), and some LiUle THINGS dwarfs, despite their low metallicity IIZw40 from Kepley+ (2014, 2016): rightmost es/mate includes H2 from ALMA; NGC5253, NGC1569, IC10 also include H2 in rightmost point dwarfs may not all be inefficient at forming stars compare with high-redshiG popula/ons, some approach maximal starbursts

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low-mass galaxy resolved HI samples

VLA-ANGST (Very Large Array survey of Advanced Camera for Surveys Nearby Galaxy Survey Treasury): 35 nearby galaxies from the ANGST survey (OU+ 2012; Warren+ 2012; S/lp+ 2013a, 2013b, 2013c) SHIELD (Survey of H I in Extremely Low-mass Dwarfs): 12 galaxies selected from the ALFALFA survey having HI masses < 107 M¤ (Cannon+ 2011; McNichols+ 2016; Teich+ 2016) FIGGS (Faint Irregular Galaxies GMRT Survey): 65 faint dwarf irregulars (dIrrs) within D≤10 Mpc (Begum+ 2008; Rowychowdhury+ 2014; Patra+ 2016) 37 dIrrs, 4 Blue Compact Dwarfs (BCDs) within D≤10.3 Mpc (Hunter+ 2007; Hunter+ 2012; Zhang+ 2012; Oh+ 2015; Maier+ 2017; Iorio, Fraternali + 2017) LITTLE THINGS (Local Irregulars That Trace Luminosity Extremes, The H I Nearby Galaxy Survey):

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low-mass galaxy resolved HI samples

Low-metallicity starbursts: 18 BCDs with measured star-forma/on histories (Lelli, Fraternali+ 2012a, 2012b, 2014a, 2014b); 18 BCDs with single-dish CO(1-0) IRAM detec/ons (Hunt+ 2015, in prep)

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low-mass starbursts: scaling rela/ons of metallicity (O/H), star- forma/on rate (SFR), stellar mass (Mstar), and gas frac/ons

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SLIDE 16

7.5 8.0 8.5 9.0 10−11 10−10 10−9 10−8 10−7

12+Log(O/H) SFR/Mstar

  • 106 107 108 109 1010 1011

Mstar

  • COLDGASS

LVL 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Gas fraction

local scaling rela/ons of stellar mass and SFR

Local Volume Legacy (LVL, KennicuU+ 2008, Lee+ 2009, Dale+ 2009, Cook+ 2014) within 11 Mpc COLDGASS (CO, followup of HI sample, Saintonge+ 2011, Huang+ 2014)

volume-limited samples also follow clear “main sequence” (Noeske+ 2007, Salim + 2007) of star forma/on (slope best fit to LVL sample, specific SFR SFR/Mstar: sSFR ~ Mstar

  • 0.13)
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SLIDE 17
  • 7.5

8.0 8.5 9.0 10−11 10−10 10−9 10−8 10−7

12+Log(O/H) SFR/Mstar

  • Lelli+ (2014)

Iorio+ (2017) Hunt+ (in prep)

  • NGC1569

DDO87

  • IIZw40

NGC1140 SBS0335−052 IZw18

106 107 108 109 1010 1011

Mstar

  • COLDGASS

LVL 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Gas fraction

local scaling rela/ons of stellar mass and SFR

but some galaxies (metal-poor low-mass starbursts) fall well outside the ±1σ spread of the main sequence (here shown by shaded grey area)

Local Volume Legacy (LVL, KennicuU+ 2008, Lee+ 2009, Dale+ 2009, Cook+ 2014) within 11 Mpc COLDGASS (CO, followup of HI sample, Saintonge+ 2011, Huang+ 2014)

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SLIDE 18

gas frac/ons correlate with specific SFR

  • 0.0

0.2 0.4 0.6 0.8 1.0 10−11 10−10 10−9 10−8 SFR/Mstar Mgas/Mbaryonic

  • COLDGASS

Thuan+ (2016) Lelli+ (2014) Iorio+ (2017) Teich+ (2016) Hunt+ (in prep)

Thuan+ (2016) includes single- dish HI

  • bserva/ons of

extremely metal- poor (XMP) dwarf galaxies, all of which are extremely gas rich

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SLIDE 19
  • 7.5

8.0 8.5 9.0 0.0 0.2 0.4 0.6 0.8 1.0

12+Log(O/H) Mgas/Mbaryonic

  • Thuan+ (2016)

Lelli+ (2014) Iorio+ (2017) Hunt+ (in prep)

  • 106

107 108 109 1010 1011

Mstar

  • COLDGASS

gas frac/ons also correlate with Mstar (less so with O/H)

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feedback and the baryonic Tully-Fisher rela/on (BTFR)

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  • 101

102 106 107 108 109 1010 1011 Vrot [km s−1] Mbaryonic [Msun]

NGC5253 NGC4163 UGC6456 SBS1415+437 NGC4449

  • Bradford+ (2015)

Lelli+ (2014) Lelli+ (2016) McGaugh (2012) Iorio+ (2017) McNichols+ (2016) Hunt+ (in prep)

Reyes+ (2011) Lelli+ (2016)

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Gas fraction

HI samples follow a fairly /ght baryonic TFR over 5 orders

  • f magnitude in mass

Hunt+ (in prep)

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SLIDE 22
  • 101

102 106 107 108 109 1010 1011 Vrot [km s−1] Mbaryonic [Msun]

NGC5253 NGC4163 UGC6456 SBS1415+437 NGC4449

  • Bradford+ (2015)

Lelli+ (2014) Lelli+ (2016) McGaugh (2012) Iorio+ (2017) McNichols+ (2016) Hunt+ (in prep)

Reyes+ (2011) Lelli+ (2016)

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Gas fraction

no/ce effect of adding molecular gas mass es/mated from CO (here included)

Hunt+ (in prep)

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feedback affects the BTFR by suppressing baryonic frac/ons at low mass

EAGLE/APOSTLE simula/ons (feedback via stochas/c thermal energy injec/on) by Sales+ (2017) log Vrot (km/s) log Mbaryonic (M¤) cri/cal issue where to measure Vrot?

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SLIDE 24
  • 101

102 106 107 108 109 1010 1011 Vrot [km s−1] Mbaryonic [Msun]

NGC5253 NGC4163 UGC6456 SBS1415+437 NGC4449

  • Bradford+ (2015)

Lelli+ (2014) Lelli+ (2016) McGaugh (2012) Iorio+ (2017) McNichols+ (2016) Hunt+ (in prep)

Sales+ (2017) EAGLE/APOSTLE Reyes+ (2011) Lelli+ (2016)

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Gas fraction

steepening of slope at low masses encompasses this feedback effect, data inconsistent with predic/on

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SLIDE 25
  • 101

102 106 107 108 109 1010 1011 Vrot [km s−1] Mbaryonic [Msun]

NGC5253 NGC4163 UGC6456 SBS1415+437 NGC4449

  • Bradford+ (2015)

Lelli+ (2014) Lelli+ (2016) McGaugh (2012) Iorio+ (2017) McNichols+ (2016) Hunt+ (in prep)

Sales+ (2017) EAGLE/APOSTLE Reyes+ (2011) Lelli+ (2016)

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Gas fraction

correc/on for pressure support* brings some points closer to correla/on

NGC 5253, NGC 4449, SBS1415+437 all contain ionized-gas

  • u}lows

(Heckman+ 2015, 2016; Chisholm+ 2015, 2016): trouble with feedback! Is Vrot truly tracing halo virializa/on? *correc/on =

√(Vrot

2 + 2 σ2) (e.g.,

Genzel 2010)

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SLIDE 26

log Vrot (km/s) log M* (M¤) mass of disk transi/on

similar behavior in Hα STELLAR TFR at z~0.2 corrected by “kinema/c parameter”: S0.5 = √(0.5 Vrot

2 + σ2), see Simons, Kassin+

(2015)

109.5 M¤

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pressure support and turbulence in low-mass galaxies : comparison of different gas tracers

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Wisnioski+ (2015), see also Green+ (2010, 2014) Moiseev+ (2015) While Hα traces rota/on through central velocity posi/on, it does not trace true turbulence in the gas, but rather bulk mo/ons of the individual HII regions unresolved spa/ally

energy injected into the ISM by star forma/on drives (ionized) gas turbulence

Log(SFR) Log[L(Hα)] σ (km/s) velocity dispersion σ correlates with SFR in dwarf galaxies, giant spirals, U/LIRGs σ also increases with redshiG (because of increasing gas frac/ons, but remember scaling rela/ons, sSFR)

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UGC8508 DDO53

  • 10−3

10−2 10−1 100 101 102 SFR [Msun yr−1] σHI [km s−1] SFR ~ σ5.3

  • Moiseev+ (2015) (ionized gas)

Lelli+ (2014) Iorio+ (2017) McNichols+ (2016)

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Gas fraction

HI velocity dispersions roughly constant with SFR

HI velocity dispersions do not show same correla/on with SFR as ionized gas

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UGC8508 DDO53

  • 10−3

10−2 10−1 100 101 102 SFR [Msun yr−1] σHI [km s−1] SFR ~ σ5.3

  • Moiseev+ (2015) (ionized gas)

Lelli+ (2014) Iorio+ (2017) McNichols+ (2016)

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Gas fraction

HI velocity dispersions do not show same correla/on with SFR as ionized gas

two galaxies currently with HI and Hα velocity dispersions measured, HI always lower

HI velocity dispersions roughly constant with SFR

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White+ (2017): CO measurements of DYNAMO galaxies at z~0.2 selected for high SFRs as local analogues for z~2 clumpy disks

  • 10−1

100 10−1 100 Mgas/Mbaryonic σ/Vrot

NGC5253

  • Lelli+ (2014)

Iorio+ (2017) McNichols+ (2016) Q = 1 (White+ 2017)

HI dwarf samples (starbursts, LITTLE THINGS, SHIELD): HI velocity dispersion rela/vely constant with gas frac/on

CO velocity dispersions increase with gas frac/on

but sample selec/on effects?

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SLIDE 32

Mogotski+ 2016 Caldu-Primo+ 2013

CO velocity dispersions ≈ HI velocity dispersions

THINGS galaxies: stacking spa/ally-

resolved spectra gives mean ra/o σ(HI)/σ(CO) = 1.0 ± 0.2 (Caldu-Primo+ 2013) Focusing on bright molecular regions gives σ(HI)/σ(CO) = 1.4 ± 0.2 (Mogotski+ 2016) Evidence for high velocity-dispersion (“thick”) molecular disk

σ(HI)/σ(CO)

σ(HI)/σ(CO)

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A cau/onary tale: global versus (too much) detail

Mrk 206 (0.2 Z¤, 12+Log(O/H) = 8.07, SMC-like) with molecular gas [CO(1-0)] observa/ons with PdBI: CO peak offset from

  • p/cal center

integrated intensity CO(1-0) SDSS thumbprint, dwarf S0

Hunt, Garcia-Burillo, Combes, et al. , in prep

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SLIDE 34

Mrk 206: regularly rota/ng disk, but lopsided σ(CO)

color Vrot color σ(CO)

high CO velocity dispersion (~ 40 km/s) coincides with highest dust ex/nc/on (Cairos+ 2010)

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Theore/cal considera/ons suggest that low-mass (metal-poor) dwarf galaxies are forming stars inefficiently, because of the impact of feedback KS rela/on suggests that this is not generally true and that some low-mass galaxies can form stars as efficiently as high-z massive starbursts Gas frac/ons in low-mass galaxies correlate with Mstar and specific SFR, and are comparable with high-z galaxies Baryonic TFR of low-mass galaxies inconsistent with theore/cal ΛCDM predic/ons, but adding a correc/on for pressure support/turbulence could beUer align results Beware of different tracers of gas velocity dispersion (ionized, molecular, atomic) as they do not probe the same physical processes To test galaxy forma/on schemes, HI measurements of rota/on/dispersion veloci/es are needed for low-mass galaxies: APERTIF, MEERKAT, SKA.

conclusions