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docs/_build/html/2303.12101.md

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<div id="title">
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# Stellar associations powering $\HII$ regions -- I. Defining an evolutionary sequence
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<div id="comments">
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[![arXiv](https://img.shields.io/badge/arXiv-2303.12101-b31b1b.svg)](https://arxiv.org/abs/2303.12101)<mark>Appeared on: 2023-03-23</mark> - _15 pages, 12 figures. Accepted for publication in MNRAS_
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</div>
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<div id="authors">
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Fabian Scheuermann, et al. -- incl., <mark><mark>Kathryn Kreckel</mark></mark>, <mark><mark>Stephen Hannon</mark></mark>, <mark><mark>Janice C. Lee</mark></mark>, <mark><mark>Frank Bigiel</mark></mark>, <mark><mark>Eva Schinnerer</mark></mark>
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</div>
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<div id="abstract">
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**Abstract:** Connecting the gas in $\HII$ regions to the underlying source of the ionizing radiation can help us constrain the physical processes of stellar feedback and how $\HII$ regions evolve over time.With PHANGS--MUSE we detect nearly $\num{24000}$ $\HII$ regions across 19 galaxies and measure the physical properties of the ionized gas (e.g. metallicity, ionization parameter, density).We use catalogues of multi-scale stellar associations from PHANGS-- $_HST_$ to obtain constraints on the age of the ionizing sources.We construct a matched catalogue of $\num{4177}$ $\HII$ regions that are clearly linked to a single ionizing association.A weak anti-correlation is observed between the association ages and the $\HA$ equivalent width $\EW$ , the $\HA/\FUV$ flux ratio and the ionization parameter, $\log q$ .As all three are expected to decrease as the stellar population ages, this could indicate that we observe an evolutionary sequence.This interpretation is further supported by correlations between all three properties.Interpreting these as evolutionary tracers, we find younger nebulae to be more attenuated by dust and closer to giant molecular clouds, in line with recent models of feedback-regulated star formation.We also observe strong correlations with the local metallicity variations and all three proposed age tracers, suggestive of star formation preferentially occurring in locations of locally enhanced metallicity.Overall, $\EW$ and $\log q$ show the most consistent trends and appear to be most reliable tracers for the age of an $\HII$ region.
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# The gas mass reservoir of quiescent galaxies at cosmic noon
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[![arXiv](https://img.shields.io/badge/arXiv-2303.12110-b31b1b.svg)](https://arxiv.org/abs/2303.12110)<mark>Appeared on: 2023-03-23</mark> - _Accepted to A&A on the 16/03/2023_
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</div>
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<div id="authors">
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David Blánquez-Sesé, et al. -- incl., <mark>E. Schinnerer</mark>
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</div>
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<div id="abstract">
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**Abstract:** We present a 1.1mm stacking analysis of moderately massive (log( $\Mstar$ / $\Msol$ ) = 10.7 $\pm$ 0.2) quiescent galaxies (QGs) at $\langle z\rangle \sim1.5$ , searching for cold dust continuum emission, an excellent tracer of dust and gas mass. Using both the recent GOODS-ALMA survey as well as the full suite of ALMA Band-6 ancillary data in the GOODS-S field, we report the tentative detection of dust continuum equivalent of dust mass log( $\Mdust$ / $\Msol$ ) = 7.47 $\pm$ 0.13 and gas mass log( $\Mgas$ / $\Msol$ ) = 9.42 $\pm$ 0.14. The emerging gas fraction is $\fgas$ = 5.3 $\pm$ 1.8 \% , consistent with the results of previous stacking analyses based on lower resolution sub(mm) observations. Our results support the scenario where high $-z$ QGs have an order of magnitude larger $\fgas$ compared to their local counterparts and have experienced quenching with a non negligible gas reservoir in their interstellar medium - i.e. with gas retention. Subsequent analysis yields an anti-correlation between the $\fgas$ and the stellar mass of QGs, especially in the high mass end where galaxies reside in the most massive haloes. The $\fgas$ - $\Mstar$ anti-correlation promotes the selection bias as a possible solution to the tension between the stacking results pointing towards gas retention in high $-z$ QGs of moderate $\Mstar$ and the studies of individual targets that favour a fully depleted ISM in massive (log( $\Mstar$ / $\Msol$ ) > 11.2) high $-z$ QGs.
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<img src="tmp_2303.12110/./Figures/f_gas_final.png" alt="Fig6.1" width="50%"/><img src="tmp_2303.12110/./Figures/fgas_mstar_15.0.png" alt="Fig6.2" width="50%"/>
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**Figure 6. -** **Gas and dust fractions of QGs**_Top_: Selection of $\fdust$ and $\fgas$ measurements as a function of redshift for QGs. Circles correspond to dust derived gas fractions: this work and previous stacks studies ($\Gobat$ and $\Magdis$) are shown in red and blue, respectively. The white circles show two different estimates (connected by a grey dotted line) for a sample of individually observed lensed galaxies. The lower values correspond to those presented in ([Whitaker, Williams and Mowla (2021)]()) and the upper values show the new estimates provided in ([Gobat and Liu (2022)]()) . The grey diamonds represent CO derived $\fgas$ estimates ([Sargent, Daddi and Bournaud 2015](), [Bezanson, Spilker and Williams 2019](), [Williams, Spilker and Whitaker 2021]()) . The red dashed area embeds $\fgas$ measurements of local QGs obtained for the ATLAS3D sample ([Young, Bureau and Davis 2011](), [Cappellari, McDermid and Alatalo 2013](), [Davis, Young and Crocker 2014]()) . The blue shaded area and the purple dashed line represent the best fit to the $\Magdis$ data and the ([Gobat, Magdis and Valentino (2020)]()) model respectively. For reference, we add the $\fgas$ evolution of main sequence galaxies according to ([Liu, Lang and Magnelli (2019)]()) . _Bottom_: Dust and gas fraction as a function of stellar mass for measurements at $z \sim 1.5$. The symbols are the same as in the top panel. The dotted line shows the $\fgas$ prediction according to the ([Davé, Finlator and Oppenheimer (2012)]()) galaxy evolution models, color coded as a function of $M_{\mathrm{halo}}$. For reference, we add the $\fgas$ - $\Mstar$ trend measured by ([Magdis, Daddi and Béthermin (2012)](), [Liu, Lang and Magnelli (2019)]()) . The light yellow scattered diamonds and arrows mark the $\fgas$ detections and upper limits for local QGs with the corresponding best fit plotted as a black dashed line. (*fig:f_gas_plot*)
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<img src="tmp_2303.12110/./Figures/Galaxy_selection_2.png" alt="Fig1" width="100%"/>
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**Figure 1. -** **Galaxy selection.** Density plot of the used ZFOURGE catalogue in the redshift vs stellar mass plane, consisting of a total 13299 galaxies. The red shaded area represents the region covered by our redshift and stellar mass selection criteria ($1 < z < 3$ and 10.20 $<$ log($\Mstar$/$\Msol$) $<$ 11.50) embedding 852 sources. The orange circles correspond to the QGs that constitute our final selection. (*fig:galaxy_selection*)
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<img src="tmp_2303.12110/./Figures/UVJ_diagram.png" alt="Fig2" width="100%"/>
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**Figure 2. -** **UVJ colour diagram.** Distribution of the parent sample of 435 galaxies that meet our selection criteria in the $U-V$, $V-J$ colour-colour space, colour coded by their log(SFR). The red box represents the quiescent region limits defined in ([Schreiber, Pannella and Elbaz (2015)]()) , which enclose the 140 QGs from which we draw our final sample. (*fig:UVJ_diagram*)
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