19 research outputs found
Giant molecular clouds under the influence of the galactic environment
The vast majority of star formation in galaxies begins in cold, dense, fractally-structured reservoirs of molecular hydrogen known as giant molecular clouds. The instantaneous
properties of these clouds and the time-scales on which they evolve can therefore be built up into models of the empirical properties of galactic-scale star formation, and so can be used to understand this process. In this thesis, we first propose a simple analytic framework to quantify the expected variation in the physical properties and lifetimes of giant molecular clouds in response to changes in their galactic-dynamical environments, finding that they vary within a fundamental parameter space spanned by the orbital angular velocity of the host galaxy, the degree of galactic shearing, the gravitational stability, and the mid-plane hydrostatic pressure. We then explore this parameter space using a set of high-resolution numerical simulations of Milky Way-like galaxies. Due to their high densities and pressures relative to the galactic mid-plane, we find that giant molecular clouds in Milky Way-like galaxies are self-gravitating and decoupled from galactic dynamics, by contrast to their lower-density progenitor clouds of atomic gas, which display systematic, galactic-dynamical variations. Finally, we analyse the full evolutionary history of each simulated cloud population as a function of the cloud spatial scale. Across all Milky Way-like environments, we find that the lifetimes of self-gravitating clouds decrease with their spatial scale below the scale-height of the thin gas disc of the galaxy, and converge to the disc crossing time at its scale-height
On the scale-height of the molecular gas disc in Milky Way-like galaxies
We study the relationship between the scale-height of the molecular gas disc
and the turbulent velocity dispersion of the molecular interstellar medium
within a simulation of a Milky Way-like galaxy in the moving-mesh code Arepo.
We find that the vertical distribution of molecular gas can be described by a
Gaussian function with a uniform scale-height of ~50 pc. We investigate whether
this scale-height is consistent with a state of hydrostatic balance between
gravity and turbulent pressure. We find that the hydrostatic prediction using
the total turbulent velocity dispersion (as one would measure from kpc-scale
observations) gives an over-estimate of the true molecular disc scale-height.
The hydrostatic prediction using the velocity dispersion between the centroids
of discrete giant molecular clouds (cloud-cloud velocity dispersion) leads to
more-accurate estimates. The velocity dispersion internal to molecular clouds
is elevated by the locally-enhanced gravitational field. Our results suggest
that observations of molecular gas need to reach the scale of individual
molecular clouds in order to accurately determine the molecular disc
scale-height.Comment: MNRAS accepted, comments welcome. 14 pages, 10 figure
Clouds of Theseus: long-lived molecular clouds are composed of short-lived H2 molecules
We use passive gas tracer particles in an Arepo simulation of a dwarf spiral
galaxy to relate the Lagrangian evolution of star-forming gas parcels and their
H2 molecules to the evolution of their host giant molecular clouds. We find
that the median chemical lifetime of H2 is just 4 Myr, independent of the
lifetime of its host molecular cloud, which may vary from 1 to 90 Myr, with a
substantial portion of all star formation in the galaxy occurring in relatively
long-lived clouds. The rapid ejection of gas from around young massive stars by
early stellar feedback is responsible for this short H2 survival time, driving
down the density of the surrounding gas, so that its H2 molecules are
dissociated by the interstellar radiation field. This ejection of gas from the
H2-dominated state is balanced by the constant accretion of new gas from the
galactic environment, constituting a "competition model" for molecular cloud
evolution. Gas ejection occurs at a rate that is proportional to the molecular
cloud mass, so that the cloud lifetime is determined by the accretion rate,
which may be as high as 4 x 10^4 Msol/Myr in the longest-lived clouds. Our
findings therefore resolve the conflict between observations of rapid gas
ejection around young massive stars and observations of long-lived molecular
clouds in galaxies, that often survive up to several tens of Myr. We show that
the fastest-accreting, longest-lived, highest-mass clouds drive supernova
clustering on sub-cloud scales, which in turn is a key driver of galactic
outflows.Comment: 16 pages, 16 figures. Submitted to MNRAS, comments welcome
The lifecycle of molecular clouds in nearby star-forming disc galaxies
It remains a major challenge to derive a theory of cloud-scale (â âČ100âpc) star formation and feedback, describing how galaxies convert gas into stars as a function of the galactic environment. Progress has been hampered by a lack of robust empirical constraints on the giant molecular cloud (GMC) lifecycle. We address this problem by systematically applying a new statistical method for measuring the evolutionary timeline of the GMC lifecycle, star formation, and feedback to a sample of nine nearby disc galaxies, observed as part of the PHANGS-ALMA survey. We measure the spatially resolved (âŒ100âpc) CO-to-Hâα flux ratio and find a universal de-correlation between molecular gas and young stars on GMC scales, allowing us to quantify the underlying evolutionary timeline. GMC lifetimes are short, typically 10â30Myrâ , and exhibit environmental variation, between and within galaxies. At kpc-scale molecular gas surface densities ÎŁH2â„8Mâpcâ2â , the GMC lifetime correlates with time-scales for galactic dynamical processes, whereas at ÎŁH2â€8Mâpcâ2 GMCs decouple from galactic dynamics and live for an internal dynamical time-scale. After a long inert phase without massive star formation traced by Hâα (75-90 perâcent of the cloud lifetime), GMCs disperse within just 1â5Myr once massive stars emerge. The dispersal is most likely due to early stellar feedback, causing GMCs to achieve integrated star formation efficiencies of 4-10 perâcent. These results show that galactic star formation is governed by cloud-scale, environmentally dependent, dynamical processes driving rapid evolutionary cycling. GMCs and HâII regions are the fundamental units undergoing these lifecycles, with mean separations of 100â300pc in star-forming discs. Future work should characterize the multiscale physics and mass flows driving these lifecycles.MC and JMDK gratefully acknowledge funding
from the Deutsche Forschungsgemeinschaft (DFG, German
Research Foundation) through an Emmy Noether Research Group
(grant number KR4801/1-1) and the DFG Sachbeihilfe (grant
number KR4801/2-1). JMDK, APSH, SMRJ, and DTH gratefully
acknowledge funding from the European Research Council
(ERC) under the European Unionâs Horizon 2020 research and
innovation programme via the ERC Starting Grant MUSTANG
(grant agreement number 714907). MC, JMDK, SMRJ, and DTH
acknowledge support from the Australia-Germany Joint Research
Cooperation Scheme (UA-DAAD, grant number 57387355).
APSH, SMRJ, and DTH are fellows of the International Max
Planck Research School for Astronomy and Cosmic Physics
at the University of Heidelberg (IMPRS-HD). BG gratefully
acknowledges the support of the Australian Research Council
as the recipient of a Future Fellowship (FT140101202). CNC,
AH, and JP acknowledge funding from the Programme National
âPhysique et Chimie du Milieu Interstellaireâ (PCMI) of the Centre
national de la recherche scientifique/Institut national des sciences
de lâUnivers (CNRS/INSU) with the Institut de Chimie/Institut de
Physique (INC/INP), co-funded by the Commissariat a lâ ` energie ÂŽ
atomique et aux energies alternatives (CEA) and the Centre ÂŽ
national dâetudes spatiales (CNES). AH acknowledges support ÂŽ
by the Programme National Cosmology et Galaxies (PNCG) of
CNRS/INSU with the INP and the Institut national de physique
nucleaire et de physique des particules (IN2P3), co-funded by ÂŽ
CEA and CNES. PL, ES, CF, DL, and TS acknowledge funding
from the ERC under the European Unionâs Horizon 2020 research
and innovation programme (grant agreement No. 694343).
The work of AKL, JS, and DU is partially supported by the
National Science Foundation (NSF) under Grants No. 1615105,
1615109, and 1653300. AKL also acknowledges partial support
from the National Aeronautics and Space Administration
(NASA) Astrophysics Data Analysis Program (ADAP) grants
NNX16AF48G and NNX17AF39G. ER acknowledges the support
of the Natural Sciences and Engineering Research Council of
Canada (NSERC), funding reference number RGPIN-2017-03987.
FB acknowledges funding from the ERC under the European
Unionâs Horizon 2020 research and innovation programme (grant
agreement No. 726384). GB is supported by the Fondo de Fomento
al Desarrollo CientŽıfico y Tecnologico of the Comisi Ž on Nacional de Ž
Investigacion Cient Ž Žıfica y Tecnologica (CONICYT/FONDECYT), Ž
Programa de Iniciacion, Folio 11150220. SCOG acknowledges ÂŽ
support from the DFG via SFB 881 âThe Milky Way Systemâ
(subprojects B1, B2, and B8) and also via Germanyâs
Excellence Strategy EXC-2181/1â390900948 (the Heidelberg
STRUCTURES Excellence Cluster). KK gratefully acknowledges
funding from the DFG in the form of an Emmy Noether
Research Group (grant number KR4598/2-1, PI Kreckel). AU
acknowledges support from the Spanish funding grants AYA2016-79006-P (MINECO/FEDER) and PGC2018-094671-B-I00
(MCIU/AEI/FEDER)
The lifecycle of molecular clouds in nearby star-forming disc galaxies
It remains a major challenge to derive a theory of cloud-scale (â âČ100âpc) star formation and feedback, describing how galaxies convert gas into stars as a function of the galactic environment. Progress has been hampered by a lack of robust empirical constraints on the giant molecular cloud (GMC) lifecycle. We address this problem by systematically applying a new statistical method for measuring the evolutionary timeline of the GMC lifecycle, star formation, and feedback to a sample of nine nearby disc galaxies, observed as part of the PHANGS-ALMA survey. We measure the spatially resolved (âŒ100âpc) CO-to-Hâα flux ratio and find a universal de-correlation between molecular gas and young stars on GMC scales, allowing us to quantify the underlying evolutionary timeline. GMC lifetimes are short, typically 10â30 Myrâ , and exhibit environmental variation, between and within galaxies. At kpc-scale molecular gas surface densities ÎŁ_(Hâ) â„ 8 M_â pcâ»ÂČâ , the GMC lifetime correlates with time-scales for galactic dynamical processes, whereas at ÎŁ_(Hâ) †8 M_â pcâ»ÂČ GMCs decouple from galactic dynamics and live for an internal dynamical time-scale. After a long inert phase without massive star formation traced by Hâα (75â90 perâcent of the cloud lifetime), GMCs disperse within just 1â5 Myr once massive stars emerge. The dispersal is most likely due to early stellar feedback, causing GMCs to achieve integrated star formation efficiencies of 4â10 perâcent. These results show that galactic star formation is governed by cloud-scale, environmentally dependent, dynamical processes driving rapid evolutionary cycling. GMCs and HâII regions are the fundamental units undergoing these lifecycles, with mean separations of 100â300 pc in star-forming discs. Future work should characterize the multiscale physics and mass flows driving these lifecycles
WISDOM project XX. - Strong shear tearing molecular clouds apart in NGC 524
Early-type galaxies (ETGs) are known to harbour dense spheroids of stars but scarce star formation (SF). Approximately a quarter of these galaxies have rich molecular gas reservoirs yet do not form stars efficiently. We study here the ETG NGC 524, with strong shear suspected to result in a smooth molecular gas disc and low star-formation efficiency (SFE). We present new spatially resolved observations of the 12CO(2-1)-emitting cold molecular gas from the Atacama Large Millimeter/sub-millimeter Array (ALMA) and of the warm ionized-gas emission lines from SITELLE at the CanadaâFranceâHawaii Telescope. Although constrained by the resolution of the ALMA observations (â37 pc), we identify only 52 GMCs with radii ranging from 30 to 140âpc, a low mean molecular gas mass surface density â©ÎŁgasâȘ â 125âMââpcâ2 and a high mean virial parameter â©Î±obs, virâȘ â 5.3. We measure spatially resolved molecular gas depletion times (Ïdep ⥠1/SFE) with a spatial resolution of â100âpc within a galactocentric distance of 1.5âkpc. The global depletion time is â2.0âGyr but Ïdep increases towards the galaxy centre, with a maximum Ïdep, max â 5.2âGyr. However, no pure HâII region is identified in NGC 524 using ionized-gas emission-line ratio diagnostics, so the Ïdep inferred are in fact lower limits. Measuring the GMC properties and dynamical states, we conclude that shear is the dominant mechanism shaping the molecular gas properties and regulating SF in NGC 524. This is supported by analogous analyses of the GMCs in a simulated ETG similar to NGC 524
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PHANGS-JWST First Results: Spurring on Star Formation: JWST Reveals Localized Star Formation in a Spiral Arm Spur of NGC 628
We combine JWST observations with Atacama Large Millimeter/submillimeter Array CO and Very Large Telescope MUSE Hα data to examine off-spiral arm star formation in the face-on, grand-design spiral galaxy NGC 628. We focus on the northern spiral arm, around a galactocentric radius of 3-4 kpc, and study two spurs. These form an interesting contrast, as one is CO-rich and one CO-poor, and they have a maximum azimuthal offset in MIRI 21 ÎŒm and MUSE Hα of around 40° (CO-rich) and 55° (CO-poor) from the spiral arm. The star formation rate is higher in the regions of the spurs near spiral arms, but the star formation efficiency appears relatively constant. Given the spiral pattern speed and rotation curve of this galaxy and assuming material exiting the arms undergoes purely circular motion, these offsets would be reached in 100-150 Myr, significantly longer than the 21 ÎŒm and Hα star formation timescales (both < 10 Myr). The invariance of the star formation efficiency in the spurs versus the spiral arms indicates massive star formation is not only triggered in spiral arms, and cannot simply occur in the arms and then drift away from the wave pattern. These early JWST results show that in situ star formation likely occurs in the spurs, and that the observed young stars are not simply the âleftoversâ of stellar birth in the spiral arms. The excellent physical resolution and sensitivity that JWST can attain in nearby galaxies will well resolve individual star-forming regions and help us to better understand the earliest phases of star formation