2021
DOI: 10.1051/0004-6361/202040010
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The VLT-MUSE and ALMA view of the MACS 1931.8-2635 brightest cluster galaxy

Abstract: We reveal the importance of ongoing in situ star formation in the brightest cluster galaxy (BCG) in the massive cool-core CLASH cluster MACS 1931.8-2635 at a redshift of z = 0.35 by analysing archival VLT-MUSE optical integral field spectroscopy. Using a multi-wavelength approach, we assessed the stellar and warm ionised medium components, which were spatially resolved by the VLT-MUSE spectroscopy, and linked them to the molecular gas by incorporating sub-mm ALMA observations. We measured the fluxes of strong … Show more

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Cited by 10 publications
(10 citation statements)
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“…The models were created using the CLOUDY code version 17.0 (Ferland 2017) for metallicities Z/Z ⊙ = 0.2, 0.5, 0.75, 1.0, 2.0 and 3.0 and ionisation parameters U 2 in the range of -4.0 ≤ log(U) ≤ -0.5 in steps of 0.5 dex. Their assumed density of n e 500 cm −3 is typical for BCGs (e.g., Ciocan et al 2021) and it is compatible with our values from Section 3.4. In both cases, most galaxies in our sample lie in the region between Z/Z ⊙ = 0.75 (12 + log(O/H)= 8.56) and Z/Z ⊙ = 1 (12 + log(O/H) = 8.69).…”
Section: Ionisation Mechanismssupporting
confidence: 88%
“…The models were created using the CLOUDY code version 17.0 (Ferland 2017) for metallicities Z/Z ⊙ = 0.2, 0.5, 0.75, 1.0, 2.0 and 3.0 and ionisation parameters U 2 in the range of -4.0 ≤ log(U) ≤ -0.5 in steps of 0.5 dex. Their assumed density of n e 500 cm −3 is typical for BCGs (e.g., Ciocan et al 2021) and it is compatible with our values from Section 3.4. In both cases, most galaxies in our sample lie in the region between Z/Z ⊙ = 0.75 (12 + log(O/H)= 8.56) and Z/Z ⊙ = 1 (12 + log(O/H) = 8.69).…”
Section: Ionisation Mechanismssupporting
confidence: 88%
“…In the "stimulated feedback" model (e.g., McNamara et al 2016), thermally unstable cooling happens in situ when warm (∼1 keV) X-ray gas is uplifted in the wake of AGNinflated radio bubbles as they rise buoyantly out of the central cluster potential, which increases the infall time and promotes the condensation of cold gas (see also Pope et al 2010). Evidence for this phenomenon has been provided in a number of systems where large reservoirs (∼10 10 M e ) of cold (10-100 K) molecular gas, observed with the Atacama Large Millimeter/submillimeter Array (ALMA), are projected behind or draped around the location of X-ray cavities as seen by Chandra (e.g., A1835: McNamara et al 2014Phoenix: Russell et al 2017a;MACS 1931.8-2634: Ciocan et al 2021A1664: Calzadilla et al 2019PKS 0745-191: Russell et al 2016;A2597: Tremblay et al 2018A1795: Russell et al 2017b2A 0335+096: Vantyghem et al 2016). On the other hand, several systems show cold gas in hot halos, even without a direct correlation with bubbles (e.g., Temi et al 2018;Olivares et al 2019;Rose et al 2019;Maccagni et al 2021;North et al 2021;McKinley et al 2022).…”
Section: Introductionmentioning
confidence: 98%
“…Most of the studies related to the origin of the cold gas have focused principally on the most massive and brightest elliptical galaxies located at the core of galaxy clusters, so-called brightest cluster galaxies. Observations of the ionized gas in galaxy clusters, traced with the Hα emission line, show spectacular filamentary structures extending up to ∼70 kpc from the core of the central galaxy (e.g., Heckman et al 1989;Hatch et al 2007;Mc-Donald et al 2010, 2011bHamer et al 2016;Hamer et al 2018;Tremblay et al 2018;Olivares et al 2019;Ciocan et al 2021). Systems with nebular emission, cold molecular gas, and ongoing star formation are preferentially found in galaxy clusters with short central cooling times, 1 Gyr and low central entropy values, 30 keV cm 2 (e.g., Cavagnolo et al 2008;Bildfell et al 2008;Pipino et al 2009;Rafferty et al 2008a;Pulido et al 2018;Loubser et al 2016).…”
Section: Introductionmentioning
confidence: 99%