Abstract:We present Atacama Large Millimeter/submillimeter Array (ALMA) imaging of molecular gas across the full star-forming disk of the barred spiral galaxy M83 in CO(J = 1–0). We jointly deconvolve the data from ALMA’s 12 m, 7 m, and Total Power arrays using the MIRIAD package. The data have a mass sensitivity and resolution of 104
M
⊙ (3σ) and 40 pc—sufficient to detect and resolve a typical molecular cloud in the Milky Way with a mass and diameter of 4 × 105
M
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“…As a definition, we favor the full duration that the gas is molecular in molecular clouds, and hence is in a prerequisite condition for potential SF. Most cloud studies stem from interests in SF, and it is more relevant to adopt the full duration that the gas can potentially form stars as cloud lifetimes (Scoville & Hersh 1979;Koda et al 2023).…”
Section: Discussion and Summarymentioning
confidence: 99%
“…Second, molecular clouds with and without SF are unevenly distributed in galactic disks. The clouds with SF are mostly along spiral arms, and those without SF are in the interarm regions (e.g., Koda et al 2023). Given disk rotation timescales of order 200 Myr, the clouds cannot move from the interarm regions to spiral arms within the suggested short lifetimes of 5-30 Myr.…”
The “tuning-fork” (TF) analysis of CO and Hα emission has been used to estimate the lifetimes of molecular clouds in nearby galaxies. With simple model calculations, we show that this analysis does not necessarily estimate cloud lifetimes, but instead captures a duration of the cloud evolutionary cycle, from dormant to star-forming, and then back to a dormant phase. We adopt a hypothetical setup in which molecular clouds (e.g., traced in CO) live forever and form stars (e.g., H ii regions) at some frequency, which then drift away from the clouds. The TF analysis still returns a timescale for the immortal clouds. This model requires drifting motion to separate the newborn stars from the clouds, and we discuss its origin. We also discuss the physical origin of the characteristic spatial separation term in the TF analysis and a bias due to systematic error in the determination of the reference timescale.
“…As a definition, we favor the full duration that the gas is molecular in molecular clouds, and hence is in a prerequisite condition for potential SF. Most cloud studies stem from interests in SF, and it is more relevant to adopt the full duration that the gas can potentially form stars as cloud lifetimes (Scoville & Hersh 1979;Koda et al 2023).…”
Section: Discussion and Summarymentioning
confidence: 99%
“…Second, molecular clouds with and without SF are unevenly distributed in galactic disks. The clouds with SF are mostly along spiral arms, and those without SF are in the interarm regions (e.g., Koda et al 2023). Given disk rotation timescales of order 200 Myr, the clouds cannot move from the interarm regions to spiral arms within the suggested short lifetimes of 5-30 Myr.…”
The “tuning-fork” (TF) analysis of CO and Hα emission has been used to estimate the lifetimes of molecular clouds in nearby galaxies. With simple model calculations, we show that this analysis does not necessarily estimate cloud lifetimes, but instead captures a duration of the cloud evolutionary cycle, from dormant to star-forming, and then back to a dormant phase. We adopt a hypothetical setup in which molecular clouds (e.g., traced in CO) live forever and form stars (e.g., H ii regions) at some frequency, which then drift away from the clouds. The TF analysis still returns a timescale for the immortal clouds. This model requires drifting motion to separate the newborn stars from the clouds, and we discuss its origin. We also discuss the physical origin of the characteristic spatial separation term in the TF analysis and a bias due to systematic error in the determination of the reference timescale.
“…These studies have consistently shown that at ∼40-100 pc resolutions, the molecular gas in the spiral arms tends to be brighter and have higher surface densities, velocity dispersions, and pressures than the gas in interarm regions, especially when a strong bar is present (Colombo et al 2014;Sun et al 2018Sun et al , 2020Rosolowsky et al 2021;Koda et al 2023). They have also shown that the slope of the distribution of cloud masses is shallower and truncates at higher masses in the spiral arms than in the interarm regions (Rosolowsky et al 2008;Koda et al 2009;Colombo et al 2014), but that despite the greater amount of star formation in the arms, the depletion time there is not significantly shorter (Querejeta et al 2021).…”
Section: Introductionmentioning
confidence: 91%
“…Much work has been done on understanding how spiral density waves and stellar feedback impact cloud formation, collapse, and dispersal, both from simulations and from observations. There have been several surveys to study the molecular gas in nearby spiral galaxies at the scale of giant molecular clouds (GMCs), such as PAWS (the PdBI Arcsecond Whirlpool Survey), which mapped M51 in CO(1−0) at 40 pc resolution (Schinnerer et al 2013); CANON (CARMA and Nobeyama Nearby Galaxies), which mapped the inner disks of nearby spiral galaxies in CO(1−0) and enabled a focused study of molecular cloud properties using a subsample at 62-78 pc resolution (Donovan Meyer et al 2013); PHANGS-ALMA (Physics at High Angular Resolution in Nearby Galaxies-Atacama Large Millimeter/submillimeter Array), which mapped 90 galaxies in CO(2−1) at ∼100 pc resolution (Leroy et al 2021); and most recently the mapping of the barred spiral galaxy M83 in CO(1−0) at 40 pc resolution (Koda et al 2023).…”
We compare the molecular cloud properties in subgalactic regions of two galaxies, barred spiral NGC 1313, which is forming many massive clusters, and flocculent spiral NGC 7793, which is forming significantly fewer massive clusters despite having a similar star formation rate to NGC 1313. We find that there are larger variations in cloud properties between different regions within each galaxy than there are between the galaxies on a global scale, especially for NGC 1313. There are higher masses, line widths, pressures, and virial parameters in the arms of NGC 1313 and the center of NGC 7793 than in the interarm and outer regions of the galaxies. The massive cluster formation of NGC 1313 may be driven by its greater variation in environment, allowing more clouds with the necessary conditions to emerge, although no one parameter seems primarily responsible for the difference in star formation. Meanwhile NGC 7793 has clouds that are as massive and have as much kinetic energy as the clouds in the arms of NGC 1313, but have densities and pressures more similar to those in the interarm regions and so are less inclined to collapse and form stars. The cloud properties in NGC 1313 and NGC 7793 suggest that spiral arms, bars, interarm regions, and flocculent spirals each represent distinct environments with regard to molecular cloud populations. We see surprisingly little difference in surface density between the regions, suggesting that the differences in surface densities frequently seen between arm and interarm regions in lower-resolution studies are indicative of the sparsity of molecular clouds, rather than differences in their true surface density.
“…Thanks to the high resolution and sensitivity of the Atacama Large Millimeter/submillimeter Array (ALMA), CO (isotopologue) observations are now routinely possible at cloud scales in nearby galaxies (e.g., Leroy et al 2021;Davis et al 2022;Koda et al 2023;Williams et al 2023). In particular, recent studies modeling multi-CO isotopologues in nearby galaxy centers have revealed that CO opacity is the dominant driver of α CO variations (Israel 2020;Teng et al 2022Teng et al , 2023.…”
Determining how the galactic environment, especially the high gas densities and complex dynamics in bar-fed galaxy centers, alters the star formation efficiency (SFE) of molecular gas is critical to understanding galaxy evolution. However, these same physical or dynamical effects also alter the emissivity properties of CO, leading to variations in the CO-to-H2 conversion factor (α
CO) that impact the assessment of the gas column densities and thus of the SFE. To address such issues, we investigate the dependence of α
CO on the local CO velocity dispersion at 150 pc scales using a new set of dust-based α
CO measurements and propose a new α
CO prescription that accounts for CO emissivity variations across galaxies. Based on this prescription, we estimate the SFE in a sample of 65 galaxies from the PHANGS–Atacama Large Millimeter/submillimeter Array survey. We find increasing SFE toward high-surface-density regions like galaxy centers, while using a constant or metallicity-based α
CO results in a more homogeneous SFE throughout the centers and disks. Our prescription further reveals a mean molecular gas depletion time of 700 Myr in the centers of barred galaxies, which is overall three to four times shorter than in nonbarred galaxy centers or the disks. Across the galaxy disks, the depletion time is consistently around 2–3 Gyr, regardless of the choice of α
CO prescription. All together, our results suggest that the high level of star formation activity in barred centers is not simply due to an increased amount of molecular gas, but also to an enhanced SFE compared to nonbarred centers or disk regions.
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