gmc populations of nearby galaxies - home | astron · 2015. 9. 7. · e.g. koda ea (2009), egusa ea...
TRANSCRIPT
![Page 1: GMC Populations of Nearby Galaxies - Home | Astron · 2015. 9. 7. · e.g. Koda ea (2009), Egusa ea (2011) IC342 Hirota ea (2011) ~1.5 kpc Some observational evidence that GMC dynamical](https://reader035.vdocuments.mx/reader035/viewer/2022081616/5feac5c874cdaf720a143ddc/html5/thumbnails/1.jpg)
Andreas Schruba, MPE for Annie Hughes, IRAP PAWS: Adam Leroy, Dario Colombo, Eva Schinnerer, Sharon Meidt, Jerome Pety, Clare Dobbs, Gaelle Dumas, Todd Thompson, Santi Garcia-Burillo, Carsten Kramer, Karl Schuster CANON: Jin Koda, Jen Donovan-Meyer, M31: Andreas Schruba MAGMA: Tony Wong, Juergen Ott
GMC Populations of Nearby Galaxies
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Milky Way’s molecular mass is ~ 2 x109 M⊙
n ~ 100 cm-3 ➡ tff ~ 4 x 106 yr ➡ SFR ~ 500 M⊙ yr-1! Observed SFR is 0.7 to 1.5 M⊙ yr-1
• bound + long-lived e.g. Krumholz & McKee (2005)
• unbound + short-lived e.g. Dobbs et al (2011) • collapsing + short-lived e.g. (Ballesteros-Paredes et al. (2011)
Explanation depends on whether GMCs are:
Motivation
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
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A Resolved Extragalactic SF ‘Law’
log(Molecular Gas Surface Density)
log
(SFR
Sur
face
Den
sity)
stars form from molecular gas with a constant depletion time of ~2 Gyr in nearby disk galaxies
nearby galaxies
starburst, high z
compilation by H
odge et al. (2014)
slope = -1.5
Solomon et al (1987)
slope = 0.5
dN/d
Mve
locit
y di
sper
sion
log(Molecular Gas Surface Density)
mass
size
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This Talk
CARMANGC6946
MAGMA LMC
NGC253: Leroy M31: Schruba NGC4526: Utomo CANON: Donovan-Meyer M33: Druard, Gratier, Braine NGC6822: Gratier IC342: Hirota M83: Hirota
ALMA NGC628
PdBI M51
Do the properties of a GMC population depend on host galaxy properties?
Do galaxy properties & processes influence GMC formation and evolution?
Do GMC properties matter for star formation (on galactic scales)?
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Are GMC Properties Universal?
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“GMCs identified on the basis of their CO emission exhibit remarkably uniform properties from galaxy to galaxy…”
Confirmation from Local Group GMCs?
log(
CO L
umino
sity)
10 100Radius [pc]
2
6
4
1
Bolatto et al 2008
Radius [pc]10 100
vel.
disp
ersio
n [k
m/s
]
1
10
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
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But...
LMC CARMA-STING
log(Σstars) log(Radius)
log(σ v
)
log(Σ H
2)
Wong ea (2013)Hughes ea (2010)
+ clear evidence for mass evolution through spiral armse.g. Koda ea (2009), Egusa ea (2011)
IC342Hirota ea (2011)
~1.5 kpc
Some observational evidence that GMC dynamical properties (e.g. mass, linewidth) may depend on galactic environment
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
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this ‘correlation’ largely due to resolution effects
log(σ/
[km
/s])
log(Radius/[pc])
intrinsic
Size-linewidth relation: M51, M33, LMC
interarm
M33
LMC
arm Decomposition applied to CO data cubes with their original spatial and spectral resolution
Data points cluster around the resolution limits
Scaling relations obtained from composite samples must be interpreted with caution: beware observational bias
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
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at fixed size, M51 clouds still have higher σ
Hughes et al (2013b)lo
g(σ/
[km
/s])
log(Radius/[pc]) log(Radius/[pc])
log(σ/
[km
/s])
matched
Size-linewidth relation: M51, M33, LMC
interarm
M33
LMC
arm
this ‘correlation’ largely due to resolution effects
intrinsic
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R-Lco relation: Nearby Galaxies
Within M51, slope and normalisation of size-luminosity relationship varies
<Σ> at fixed scale also varies between galaxies
difference in <Σ> between spiral and dwarf galaxies (factor of ~10) exceeds XCO variations (factor of ~2 to 3)
10 100
2
4
6
log(LCO/[K km/s pc2])
M51 interarm
M33
LMC
size-luminosity
M51 arm
N6946
N4826
Radius [pc]
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015Hughes et al (2013b)
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Extragalactic Larson Relations at 50pc
Radius [pc]
log(σ/[km/s])
10 100
1
10
size-linewidth
<σ>/R and Σ of GMCs vary with galactic environment
10 100Radius [pc]
2
4
6
log(LCO/[K km/s pc2])
M51 interarm
M33
LMC
M51 arm
N6946
N4826
100
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
size-luminosity
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A consequence of external pressure?
e.g. Elmegreen (1989)
➡ if Pint~Pext, environment more likely to influence cloud stability, dense gas mass function, star formation activity, GMC evolution...
PGMC=P
ISM
PGMC=1
0PISM
PGMC=0
.1PISM
M33LMCM51
M64NGC6946
dwarfs
GMC vs ISM pressure
4 65
4
6
5
log(Pext/kB[K cm-3])
log(Pint/k B[K cm-3])
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
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How is Molecular Gas in Galaxies Distributed?
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• diagnostic of GMC formation & destruction processes • potential link to core mass function and cluster IMF • in inner MW, γ = -1.5 ➡ GMCs dominate total H2 mass
GMC Mass Distributions: Motivations
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
slope = -1.5
Solomon et al (1987)dN
/dM
cloud mass
Kruijssen (2014)
observed mass
Toom
re M
ass
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PAWS Survey of M51: Dynamical environments defined in Colombo et al (2014)
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Colombo et al (2014)
log(
N(m
>M)/[
kpc2
])
-1
2
-1
2
5 76 5 76 5 76log(Mass/M⊙)
GMC Mass Spectra: M51 environments
ARM outside CR
ARM inside CR DOWN
UP
-1.3
-1.6 -1.8
-1.8
-2.4
-2.6
RING
BAR
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GMC & Young Cluster PropertiesMass Function Slope Maximum (P95) Mass
log(Max GMC Mass)MF slope (GMCs)
MF
slope
(clus
ters
)
Log(
Max
Clus
ter M
ass) Hughes et al (2013a)
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GMC Mass Spectra: Nearby Galaxies
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
log (GMC Mass/[M⦿])
LMC M31 N628
simple power law is insufficient for most galaxies GMC mass spectra are steeper in diffuse environments
log(
N(M
* >M
)/[kp
c2 ])
M51arms
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GMC Mass Distributions: Trends
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
shape of GMC mass distribution is not universal: slope and turnover mass increase in more massive systems
M51M31LMC N628 N6946M33
Slop
eTr
unca
tion
Mas
s
Stellar Mass Σ(stars) RmolΣ(gas)
Stellar Mass Σ(stars) RmolΣ(gas)
Hughes et al (in prep)
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Do GMC properties matter for star formation (on galactic scales)?
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Star Formation: TheoryIn star formation theory, the SFR depends on the properties of the parent cloud
e.g. Krumholz & McKee 2005, Padoan & Nordlund 2011, Hennebelle & Chabrier 2011, Federrath & Klessen 2012,
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
Fede
rrath
& K
lesse
n 20
12
SFR
per f
ree-
fall
time
Padoan & Nordlund
Krumholz & McKee
Hennebelle & Chabrier
Mach Number
virial parameter
• cloud properties act as the boundary conditions for small scale star formation • turbulent cloud properties set the
density distribution • Mach number sets the width of
density distribution
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Star Formation in Local Clouds
log(Visual Extinction)
Rela
tive
Freq
uenc
y
In local clouds, SFR relates to high density gas, not total H2
• YSOs found in regions of high column density and extinction
• Actively SF clouds show excess amounts of high extinction material
• SF appears closely associated with dense filamentary substructure
Kainulainen et al (2009), Lada et al (2010), Heiderman et al (2010), Arzoumanian et al (2011), Stutz et al (2015)
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
Kainu
laine
n et
al (2
009)
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log
(SFR
Sur
face
Den
sity
)
undisturbed disks
merger + interacting
Extragalactic Star Formation
incr
easi
ng s
tella
r mas
s
log(H2 Surface Density)
SFR-per-H2 varies (systematically) on large scales in local galaxies• High SFR/CO in galaxy
centres, luminous starbursts, low-metallicity dwarfs
• Low SFR/CO in ETGs
• SFR/CO shows variations with local gas kinematics, galaxy morphology and metallicity
Schruba et al (2011), Saintonge et al (2011), Davis et al (2014), Meidt et al (2013), Koda et al (2009), Leroy et al
(2013), Gao & Solomon (2004), Huang et al (2015)
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
Schr
uba
et a
l (201
1),
Saint
onge
et a
l (201
1
SF closely related to
H2
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GMC Properties and Star Formation
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
Measure TIR/CO, SFR/HCN, or HCN/CO ratio in a ~kpc aperture that is small enough to roughly isolate local conditions.
For simplicity, we write TIR/CO: overall SFE in H2 HCN/CO: dense gas fraction TIR/HCN: SFE of dense gas
Integration over a ~kpc area is needed to capture the time-cycling of gas and stars
Schinnerer et al (2013), Pety et al (2013)
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GMC Properties and Star Formation
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
Within the ~kpc aperture, measure the typical cloud-scale properties of the molecular gas, e.g. mass-weighted surface density, velocity dispersion (Mach number), and gravitational boundedness
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Underlying GMC Properties Matter
Cloud Boundedness
TIR-
to-C
O a
t 1kp
c ~
SFE
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
Within the PAWS field-of-view, the ability of the ISM to form stars (IR/CO) correlates with the self-gravity of the gas at cloud (50 pc) scales – gas that is more bound appears better at forming stars.
more boundLe
roy,
Hugh
es, S
chinn
erer
, Big
iel (in
pre
p)
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Underlying GMC Properties Matter
H2 Surface Density
HC
N-to
-CO
at 1
kpc
~ de
nse
gas
fract
ion
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
Within the PAWS field-of-view, the average small scale surface density within a kpc region correlates with the apparent fraction of the molecular gas mass that is dense.
denserLero
y, Hu
ghes
, Sch
inner
er, B
igiel
(in p
rep)
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Underlying GMC Properties Matter
H2 Surface Density
IR-to
-HC
N a
t 1kp
c
~SFE
in d
ense
gas
Annie Hughes, IRAP ● Local Gas, ASTRON ● Sept 2015
But higher cloud-scale surface densities are associated with lower ratios of star formation per unit dense gas! I.e. dense gas is worse at forming stars as overall ISM density increases
denserLe
roy,
Hugh
es, S
chinn
erer
, Big
iel (in
pre
p)
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SummaryGMC physical properties and mass distributions vary with environment, both within and among galaxies
More massive systems tend to have denser, more turbulent GMCs, and tend to build more massive GMCs
In M51, relations between star formation, molecular gas and dense gas are qualitatively consistent with a “whole cloud” view in which star formation occurs in local overdensities (rather than a universal density threshold)