C. D. Wilson’s research while affiliated with McMaster University and other places

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Publications (162)


Fig. 3. Left: resolved KS relation for the VERTICO ensemble sample at a resolution of 720 pc. The red contours show the relation obtained for HI-deficient galaxies, according to Zabel et al. (2022), whereas the blue contours indicate the relation obtained for normal galaxies. Solid lines indicate LTS fits to the data. Similarly to Figure 2 only galaxies with i < 80 o have been considered and values for Σ SFR and Σ mol have been corrected to face-on via cosi. The plot shows longer gas depletion times for HI-deficient VERTICO galaxies. Right: SFR − M relation for the VERTICO subsample, limited to HI-deficient and HI-normal galaxies covering the same range in stellar mass. The different colors indicate HI-deficient (red) and HI-normal (blue) galaxies. Overlaid are the star formation main sequence (SFMS) relation obtained in Elbaz et al. (2007) in black (solid line), as well as that presented in xCOLD GASS in orange (Saintonge et al. 2016). While VERTICO HI-normal galaxies lie on the SFMS, HI-deficient galaxies are mostly scattered below the SFMS.
Fig. 4. HI-deficiency parameter as a function of the total stellar mass (left), global star formation rate (middle) and specific SFR (right) for each galaxy. The Pearson's correlation coefficients are shown on the different panels for each distribution. These quantities are calculated for the VERTICO sample of galaxies shown on the right panel of Figure 3.
Fig. 5. The resolved Kennicutt-Schmidt relation for the sub-sample of galaxies in the VERTICO sample with inclinations i ≤ 80 o , represented as Σ SFR as a function of Σ mol . All data points are convolved to a common working resolution of 720 pc. Each data point is color-coded by the distance to the galaxy center. The diagonal dashed, grey lines show constant depletion times of 0.1, 1 and 10 Gyr, respectively. For a fixed molecular gas mass, there are clear galaxy-to-galaxy variations in the KS relation. OLS weighted fits to the line-of-sight measurements are the solid blue lines shown in Table 4. Note that values for Σ SFR and Σ mol have been corrected via cos i.
Fig. 6. Histogram of best-fit power-law KS index, N, for individual galaxies in VERTICO (blue color, see Table 4) using a fixed CO-to-H 2 conversion factor. For a comparison, orange bars represent the subsample of HERACLES galaxies used in Leroy et al. (2013) and green bars show the best-fit slopes found for the sub-sample of PHANGS galaxies presented in Pessa et al. (2021). The distribution of best-fit N for individual galaxies in VERTICO spans the range N ∼ 0.7 − 1.5 and peaks near N = 0.9, while this value is slightly larger for the HERA-CLES and PHANGS distributions.
VERTICO III: The Kennicutt-Schmidt relation in Virgo cluster galaxies
  • Preprint
  • File available

November 2022

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57 Reads

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T. Brown

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C. D. Wilson

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[...]

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In this VERTICO science paper we aim to study how the star formation process depends on galactic environment and gravitational interactions in the context of galaxy evolution. We explore the scaling relation between the star formation rate (SFR) surface density and the molecular gas surface density, also known as the Kennicutt-Schmidt (KS) relation, in a subsample of Virgo cluster spiral galaxies. We use new ACA and TP observations from the VERTICO-ALMA Large Program at 720pc resolution to resolve the molecular gas content, as traced by the 12CO(2-1) transition, across the disks of 37 spiral galaxies in the Virgo cluster. In combination with archival observations, we estimate the parameters of the KS relation for the entire ensemble of galaxies, and within individual galaxies. We find the KS slope for the entire population to be N=0.97+/-0.07, with a characteristic molecular gas depletion time of 1.86Gyr for our full sample, in agreement with previous work in isolated star-forming galaxies. In individual galaxies, we find KS slopes ranging between 0.69 and 1.40, and typical star formation efficiencies (SFE) that can vary from galaxy to galaxy by a factor of ~4. These galaxy-to-galaxy variations account for ~0.20dex in scatter in the ensemble KS relation, which is characterized by a 0.42dex scatter. We find that the HI-deficient galaxies in the Virgo cluster show a steeper resolved KS relation and lower molecular gas efficiencies than HI-normal cluster galaxies. While the molecular gas content in Virgo cluster galaxies appears to behave similarly to that in isolated galaxies, our VERTICO sample shows that cluster environments play a key role in regulating star formation. The environmental mechanisms affecting the HI galaxy content also have a direct impact in the SFE of molecular gas in cluster galaxies, leading to longer depletion times in HI-deficient members.

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Physical properties of the ambient medium and of dense cores in the Perseus star-forming region derived from Herschel Gould Belt Survey observations

September 2020

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25 Reads

(Abridged) In this paper, we present analyses of images taken with the Herschel ESA satellite from 70mu to 500mu. We first constructed column density and dust temperature maps. Next, we identified compact cores in the maps, and characterize the cores using modified blackbody fits to their SEDs: we identified 684 starless cores, of which 199 are bound and potential prestellar cores, and 132 protostars. We also matched the Herschel-identified young stars with GAIA sources to model distance variations across the Perseus cloud. We measure a linear gradient function with right ascension and declination for the entire cloud. From the SED fits, mass and temperature of cores were derived. The core mass function can be modelled with a log-normal distribution that peaks at 0.82~M_\sun suggesting a star formation efficiency of 0.30. The high-mass tail can be modelled with a power law of slope 2.32\sim-2.32, close to the Salpeter's value. We also identify the filamentary structure of Perseus, confirming that stars form preferentially in filaments. We find that the majority of filaments where star formation is ongoing are transcritical against their own internal gravity because their linear masses are below the critical limit of 16~M_\sunpc1^{-1} above which we expect filaments to collapse. We find a possible explanation for this result, showing that a filament with a linear mass as low as 8~M_\sunpc1^{-1} can be already unstable. We confirm a linear relation between star formation efficiency and slope of dust probability density function and a similar relation is also seen with the core formation efficiency. We derive a lifetime for the prestellar core phase of 1.69±0.521.69\pm0.52~Myr for Perseus but different regions have a wide range in prestellar core fractions, hint that star-formation has started only recently in some clumps. We also derive a free-fall time for prestellar cores of 0.16~Myr.


Figure 9. The amount of dust produced through stellar sources (AGB + SNe, dashed curves) and through interstellar grain growth (solid curves) as a function of galaxy age, as inferred from the median model parameter values for Bin 4. The stardust tracks for Model I and Model III overlap due to the same assumed SFH shape for both models.
JINGLE – IV. Dust, H i gas, and metal scaling laws in the local Universe

August 2020

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53 Reads

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63 Citations

Monthly Notices of the Royal Astronomical Society

Scaling laws of dust, H i gas, and metal mass with stellar mass, specific star formation rate, and metallicity are crucial to our understanding of the build-up of galaxies through their enrichment with metals and dust. In this work, we analyse how the dust and metal content varies with specific gas mass (MH i/M⋆) across a diverse sample of 423 nearby galaxies. The observed trends are interpreted with a set of Dust and Element evolUtion modelS (DEUS) – including stellar dust production, grain growth, and dust destruction – within a Bayesian framework to enable a rigorous search of the multidimensional parameter space. We find that these scaling laws for galaxies with −1.0 ≲ log MH i/M⋆ ≲ 0 can be reproduced using closed-box models with high fractions (37–89  per cent{{\ \rm per\ cent}}) of supernova dust surviving a reverse shock, relatively low grain growth efficiencies (ϵ = 30–40), and long dust lifetimes (1–2 Gyr). The models have present-day dust masses with similar contributions from stellar sources (50–80  per cent{{\ \rm per\ cent}}) and grain growth (20–50  per cent{{\ \rm per\ cent}}). Over the entire lifetime of these galaxies, the contribution from stardust (>90  per cent{{\ \rm per\ cent}}) outweighs the fraction of dust grown in the interstellar medium (<10  per cent{{\ \rm per\ cent}}). Our results provide an alternative for the chemical evolution models that require extremely low supernova dust production efficiencies and short grain growth time-scales to reproduce local scaling laws, and could help solving the conundrum on whether or not grains can grow efficiently in the interstellar medium.


JINGLE -- IV. Dust, HI gas and metal scaling laws in the local Universe

August 2020

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41 Reads

Scaling laws of dust, H I gas, and metal mass with stellar mass, specific star formation rate, and metallicity are crucial to our understanding of the build-up of galaxies through their enrichment with metals and dust. In this work, we analyse how the dust and metal content varies with specific gas mass (MH I/M⋆) across a diverse sample of 423 nearby galaxies. The observed trends are interpreted with a set of Dust and Element evolUtion modelS (DEUS) – including stellar dust production, grain growth, and dust destruction – within a Bayesian framework to enable a rigorous search of the multidimensional parameter space. We find that these scaling laws for galaxies with −1.0 ≲ log MH I/M⋆ ≲ 0 can be reproduced using closed-box models with high fractions (37–89 per cent⁠) of supernova dust surviving a reverse shock, relatively low grain growth efficiencies (ϵ = 30–40), and long dust lifetimes (1–2 Gyr). The models have present-day dust masses with similar contributions from stellar sources (50–80 per cent⁠) and grain growth (20–50 per cent⁠). Over the entire lifetime of these galaxies, the contribution from stardust (>90 per cent⁠) outweighs the fraction of dust grown in the interstellar medium (<10 per cent⁠). Our results provide an alternative for the chemical evolution models that require extremely low supernova dust production efficiencies and short grain growth time-scales to reproduce local scaling laws, and could help solving the conundrum on whether or not grains can grow efficiently in the interstellar medium.


Figure 1. From left to right, and top to bottom: histograms of the metallicities (as traced by the oxygen abundance), stellar masses, star formation rates (SFRs), specific star formation rates (sSFRs), Hi masses (M HI ) and distances for the JINGLE (red filled histograms), HRS (green vertical lines), KINGFISH (blue diagonal lines), HAPLESS (yellow lines) and HiGH (orange diagonal lines) galaxies. Median sample values are indicated with vertical dashed lines using the same colour-coding.
Figure 9. The amount of dust produced through stellar sources (AGB+SNe, dashed curves) and through interstellar grain growth (solid curves) as a function of galaxy age, as inferred from the median model parameter values for Bin 4. The stardust tracks for Model I and Model III overlap due to the same assumed SFH shape for both models.
Figure C2. The star formation main sequence for JINGLE, HRS, KINGFISH, HAPLESS and HiGH galaxies (grey symbols), with the average trend found by Saintonge et al. (2016) overlaid as a solid black line. An offset of 0.3 dex on either side of this trend (similar to the spread observed by Noeske et al. 2007; Pannella et al. 2009; Rodighiero et al. 2010) has been indicated by dashed black lines, and encloses galaxies located on the SF main sequence. The evolutionary path for the customised and delayed SFHs have been overlaid with solid and dashed curves, respectively, for galaxy Bins 1 through to 6 in black, purple, blue, green, yellow and red. The location of the asterisk corresponds to a lookback time of 2 Gyr.
Figure G2. Corner plot for Model II (i.e., closed-box models with a delayed SFH) for galaxy bin 1. See caption of Fig. G1 for more information.
JINGLE -- IV. Dust, HI gas and metal scaling laws in the local Universe

June 2020

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318 Reads

Scaling laws of dust, HI gas and metal mass with stellar mass, specific star formation rate and metallicity are crucial to our understanding of the buildup of galaxies through their enrichment with metals and dust. In this work, we analyse how the dust and metal content varies with specific gas mass (MHIM_{\text{HI}}/MM_{\star}) across a diverse sample of 423 nearby galaxies. The observed trends are interpreted with a set of Dust and Element evolUtion modelS (DEUS) - incluidng stellar dust production, grain growth, and dust destruction - within a Bayesian framework to enable a rigorous search of the multi-dimensional parameter space. We find that these scaling laws for galaxies with 1.0logMHI-1.0\lesssim \log M_{\text{HI}}/M0M_{\star}\lesssim0 can be reproduced using closed-box models with high fractions (37-89%\%) of supernova dust surviving a reverse shock, relatively low grain growth efficiencies (ϵ\epsilon=30-40), and long dus lifetimes (1-2\,Gyr). The models have present-day dust masses with similar contributions from stellar sources (50-80\,%\%) and grain growth (20-50\,%\%). Over the entire lifetime of these galaxies, the contribution from stardust (>>90\,%\%) outweighs the fraction of dust grown in the interstellar medium (<<10%\%). Our results provide an alternative for the chemical evolution models that require extremely low supernova dust production efficiencies and short grain growth timescales to reproduce local scaling laws, and could help solving the conundrum on whether or not grains can grow efficiently in the interstellar medium.


The CO(3-2)/CO(1-0) luminosity line ratio in nearby star-forming galaxies and AGN from xCOLD GASS, BASS and SLUGS

January 2020

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14 Reads

We study the {r}_{31}={L}_{\mathrm{CO}(3\mbox{--}2)}^{{\prime} }/{L}_{\mathrm{CO}(1\mbox{--}0)}^{{\prime} } luminosity line ratio in a sample of nearby (z < 0.05) galaxies: 25 star-forming galaxies (SFGs) from the xCOLD GASS survey, 36 hard X-ray-selected active galactic nucleus (AGN) host galaxies from the BAT AGN Spectroscopic Survey, and 37 infrared-luminous galaxies from the SCUBA Local Universe Galaxy Survey. We find a trend for r 31 to increase with star formation efficiency (SFE). We model r 31 using the UCL-PDR code and find that the gas density is the main parameter responsible for the variation of r 31, while the interstellar radiation field and cosmic-ray ionization rate play only a minor role. We interpret these results to indicate a relation between SFE and gas density. We do not find a difference in the r 31 value of SFGs and AGN host galaxies, when the galaxies are matched in SSFR (〈r 31〉 = 0.52 ± 0.04 for SFGs and 〈r 31〉 = 0.53 ± 0.06 for AGN hosts). According to the results of the UCL-PDR models, the X-rays can contribute to the enhancement of the CO line ratio, but only for strong X-ray fluxes and for high gas density (n H > 104 cm−3). We find a mild tightening of the Kennicutt–Schmidt relation when we use the molecular gas mass surface density traced by CO(3–2) (Pearson correlation coefficient R = 0.83), instead of the molecular gas mass surface density traced by CO(1–0) (R = 0.78), but the increase in correlation is not statistically significant (p-value = 0.06). This suggests that the CO(3–2) line can be reliably used to study the relation between SFR and molecular gas for normal SFGs at high redshift and to compare it with studies of low-redshift galaxies, as is common practice.


SCOPE: SCUBA-2 Continuum Observations of Pre-protostellar Evolution -survey description and compact source catalogue

May 2019

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99 Reads

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39 Citations

Monthly Notices of the Royal Astronomical Society

We present the first release of the data and compact-source catalogue for the JCMT Large Program SCUBA-2 Continuum Observations of Pre-protostellar Evolution (SCOPE). SCOPE


SCOPE: SCUBA-2 Continuum Observations of Pre-protostellar Evolution - Survey Description and Compact Source Catalogue

February 2019

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121 Reads

We present the first release of the data and compact-source catalogue for the JCMT Large Program SCUBA-2 Continuum Observations of Pre-protostellar Evolution (SCOPE). SCOPE consists of 850-um continuum observations of 1235 Planck Galactic Cold Clumps (PGCCs) made with the Submillimetre Common-User Bolometer Array 2 on the James Clerk Maxwell Telescope. These data are at an angular resolution of 14.4 arcsec, significantly improving upon the 353-GHz resolution of Planck at 5 arcmin, and allowing for a catalogue of 3528 compact sources in 558 PGCCs. We find that the detected PGCCs have significant sub-structure, with 61 per cent of detected PGCCs having 3 or more compact sources, with filamentary structure also prevalent within the sample. A detection rate of 45 per cent is found across the survey, which is 95 per cent complete to Planck column densities of NH2N_{H_{2}} >> 5 ×\times 1021^{21} cm2^{-2}. By positionally associating the SCOPE compact sources with YSOs, the star formation efficiency, as measured by the ratio of luminosity to mass, in nearby clouds is found to be similar to that in the more distant Galactic Plane, with the column density distributions also indistinguishable from each other.


Comprehensive comparison of models for spectral energy distributions from 0.1 micron to 1 mm of nearby star-forming galaxies

September 2018

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121 Reads

We have fit the far-ultraviolet (FUV) to sub-millimeter (850 micron) spectral energy distributions (SEDs) of the 61 galaxies from the "Key Insights on Nearby Galaxies: A Far-Infrared Survey with Herschel" (KINGFISH). The fitting has been performed using three models: the Code for Investigating GALaxy Evolution (CIGALE), the GRAphite-SILicate approach (GRASIL), and the Multi-wavelength Analysis of Galaxy PHYSical properties (MAGPHYS). We have analyzed the results of the three codes in terms of the SED shapes, and by comparing the derived quantities with simple "recipes" for stellar mass (Mstar), star-formation rate (SFR), dust mass (Mdust), and monochromatic luminosities. Although the algorithms rely on different assumptions for star-formation history, dust attenuation and dust reprocessing, they all well approximate the observed SEDs and are in generally good agreement for the associated quantities. However, the three codes show very different behavior in the mid-infrared regime, in particular between 25 and 70 micron where there are no observational constraints for the KINGFISH sample. We find that different algorithms give discordant SFR estimates for galaxies with low specific SFR, and that the standard "recipes" for calculating FUV absorption overestimate the extinction compared to the SED-fitting results. Results also suggest that assuming a "standard" constant stellar mass-to-light ratio overestimates Mstar relative to the SED fitting, and we provide new SED-based formulations for estimating Mstar from WISE W1 (3.4 micron) luminosities and colors. From a Principal Component Analysis of Mstar, SFR, Mdust, and O/H, we reproduce previous scaling relations among Mstar, SFR, and O/H, and find that Mdust can be predicted to within roughly 0.3 dex using only Mstar and SFR.


The JCMT Gould Belt Survey: A First Look at the Auriga-California Molecular Cloud with SCUBA-2

January 2018

We present 850 and 450 micron observations of the dense regions within the Auriga-California molecular cloud using SCUBA-2 as part of the JCMT Gould Belt Legacy Survey to identify candidate protostellar objects, measure the masses of their circumstellar material (disk and envelope), and compare the star formation to that in the Orion A molecular cloud. We identify 59 candidate protostars based on the presence of compact submillimeter emission, complementing these observations with existing Herschel/SPIRE maps. Of our candidate protostars, 24 are associated with young stellar objects (YSOs) in the Spitzer and Herschel/PACS catalogs of 166 and 60 YSOs, respectively (177 unique), confirming their protostellar nature. The remaining 35 candidate protostars are in regions, particularly around LkHalpha 101, where the background cloud emission is too bright to verify or rule out the presence of the compact 70 micron emission that is expected for a protostellar source. We keep these candidate protostars in our sample but note that they may indeed be prestellar in nature. Our observations are sensitive to the high end of the mass distribution in Auriga-Cal. We find that the disparity between the richness of infrared star forming objects in Orion A and the sparsity in Auriga-Cal extends to the submillimeter, suggesting that the relative star formation rates have not varied over the Class II lifetime and that Auriga-Cal will maintain a lower star formation efficiency.


Citations (72)


... high-redshift galaxies, SNe alone are likely insufficient to account for all the observed dust in the early Universe (e.g., Michałowski 2015; Leśniewska & Michałowski 2019;Algera et al. 2024b). However, utilizing a different local galaxy sample and modeling approach, De Looze et al. (2020) infer significantly higher SN yields, highlighting that such empirical approaches remain limited by degeneracies between the various dust production and destruction processes (see also Calura et al. 2023;Park et al. 2024). ...

Reference:

REBELS-IFU: Dust Build-up in Massive Galaxies at Redshift 7
JINGLE – IV. Dust, H i gas, and metal scaling laws in the local Universe

Monthly Notices of the Royal Astronomical Society

... Clumps masses and radii are obtained as follows. Using the 870 μm and 850 μm emission from the ATLASGAL survey 11 (Schuller et al. 2009) and SCOPE survey 12 (Eden et al. 2019), we first fitted each target with a 2D Gaussian function to derive the integrated flux (S ν ) and size of the clumps. The clump radius, R cl , is calculated as the geometrical mean of the semiminor and semimajor full width at half maximum (FWHM) deconvolved from the beam. ...

SCOPE: SCUBA-2 Continuum Observations of Pre-protostellar Evolution -survey description and compact source catalogue

Monthly Notices of the Royal Astronomical Society

... Located in the Taurus-Perseus-Auriga complex (Ungerechts & Thaddeus 1987;Dame et al. 2001), the CMC is identified to be a giant molecular cloud (GMC), which is similar to the Orion Molecular Cloud (OMC) in mass (∼ 10 5 M ⊙ ) and size (∼ 80 pc), but in an earlier evolution stage (Lada et al. 2009;Broekhoven-Fiene et al. 2018). Compared with the OMC, the CMC was found to contain 15−20 times fewer young stellar objects (YSOs) in number (Broekhoven-Fiene et al. 2014). ...

The JCMT Gould Belt Survey: A First Look at the Auriga–California Molecular Cloud with SCUBA-2

The Astrophysical Journal

... ;Hailey-Dunsheath et al. 2008Panuzzo et al. 2010;Rangwala et al. 2011;Papadopoulos et al. 2012;Spinoglio et al. 2012;Meijerink et al. 2013;Pereira-Santaella et al. 2013;Rigopoulou et al. 2013;Greve et al. 2014;Kamenetzky et al. 2014Kamenetzky et al. , 2016Kamenetzky et al. , 2017Lu et al. 2014Lu et al. , 2017Rosenberg et al. 2014aRosenberg et al. , 2014bSchirm et al. 2014Schirm et al. , 2017Zhang et al. 2014;Israel et al. 2015;Liu et al. 2015;Mashian et al. 2015;Wu et al. 2015;Yang et al. 2017;Valentino et al. 2020a). A third state that is mostly responsible for J u  10 CO lines is also found in the case of AGNs (e.g.,van der Werf et al. 2010;Rangwala et al. 2011;Spinoglio et al. 2012) or mechanical heating (e.g.,Rosenberg et al. 2014a) ...

Probing the cold and warm molecular gas in the Whirlpool Galaxy: Herschel* SPIRE-FTS Observations of the central region of M51 (NGC 5194)

Monthly Notices of the Royal Astronomical Society

... Analyses of galaxy spectra reveal an unexpected excess in far-infrared (FIR), submillimetre and millimetre dust emission (known as the 'submm excess'). This excess is primarily observed in the spectral energy distributions (SEDs) of many low-metallicity galaxies [33,34,35,36,37,38,39,40], indicating a clear discrepancy between dust models and observations. Furthermore, satellite and other measurements of dust and micrometeorites in the Solar System [41,42], along with studies of asteroid distribution in the Main Asteroid Belt in the Solar System [43,44,45,46], show that the dust mass distribution in the solar neighbourhood differs significantly from that considered by standard dust models [47] and their modifications [48,49,50,51,52]. ...

Updated 34-band Photometry for the SINGS/KINGFISH Samples of Nearby Galaxies
  • Citing Article
  • March 2017

... The sources of error are a sum-in-quadrature of calibration uncertainties and background fluctuations. The results are given in Table 1, where we compare them to the results of Dale et al. 2017, who compiled photometry from 34 bands for the SINGS/KINGFISH Hershel/Spitzer sample of local galaxies. ...

Updated 34-band Photometry for the Sings/KINGFISH Samples of Nearby Galaxies
  • Citing Article
  • February 2017

The Astrophysical Journal

... Such areas with enhanced H 2 surface densities have been reported in studies of the effects of RPS on the ISM in cluster galaxies, both in observational studies (e.g. Mok et al. 2017;Cramer et al. 2020Cramer et al. , 2021Roberts et al. 2022) and simulations (e.g. Bekki 2014;Steinhauser et al. 2016;Tonnesen 2019). ...

The JCMT Nearby Galaxies Legacy Survey -- XI. -- Environmental Variations in the Atomic and Molecular Gas Radial Profiles of Nearby Spiral Galaxies
  • Citing Article
  • February 2017

Monthly Notices of the Royal Astronomical Society

... Studying the central few hundreds parsecs of the galaxy is of extreme importance to understand the formation and evolution of galaxy [1]. The processes at the center of spiral galaxy have no counterparts in the disk [2]. The densities and temperature of the molecular at the center parts are higher than that in the disk. ...

The central region of spiral galaxies as seen by Herschel

Astronomy and Astrophysics

... To best match this area, we begin by using [C II] and [O I] line fluxes measured through the central spaxel of the PACS/IFU with dimensions of ∼ 9 4 × 9 4 (See Section 3.2 in Díaz-Santos et al. 2017). Next, we project the effective SL slit and PACS central-spaxel aperture onto the Spitzer/IRAC 8 μm images, assuming that it traces the co-spatial PAH and far-IR line emission from star-forming regions in LIRGs, which is reasonable for the 2-7 kpc-scale observations in this work (Peeters et al. 2004;Alonso-Herrero et al. 2010;Pereira-Santaella et al. 2010;Hughes et al. 2016;Salgado et al. 2016). Smith et al. (2007) show the fractional power of PAHs to the IRAC 8 μm band to have a median value of 70% in normal star-forming galaxies, which increases only marginally when a more careful subtraction of stellar continuum is done using the IRAC 3-5 μm channels (e.g., Helou et al. 2004). ...

The spatially-resolved correlation between [NII] 205 {\mu}m line emission and the 24 {\mu}m continuum in nearby galaxies
  • Citing Article
  • January 2016

Astronomy and Astrophysics

... The colors of these regions are plotted in Figure 4. data. While more well known in the public health field, this analysis technique has been used for similar purposes to that we described here in a number of other astronomy papers (e.g., A. Mok et al. 2016; M. C. Odekon et al. 2016). All galaxies in our samples are detected in r, but ∼20% of the sample have an upper-limit flux in the FUV or NUV, which are important to consider as limits still provide useful color constraints. ...

The JCMT Nearby Galaxies Legacy Survey X. Environmental Effects on the Molecular Gas and Star Formation Properties of Spiral Galaxies
  • Citing Article
  • December 2015

Monthly Notices of the Royal Astronomical Society