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Cluster member galaxies with spectroscopic redshifts from Gemini identified on an SDSS r-band image. Blue boxes (red circles) denote members with higher (lower) redshifts than the systemic cluster redshift of z = 0.363. Large, bold symbols mark the BCGs of both kinematic components. The 148 GHz Compton y SZ contours are superposed. The contours start at a level of 2.0 × 10 −5 , increasing towards the centre in steps of 1.25 × 10 −5. The black X marks the cluster SZ peak.

Cluster member galaxies with spectroscopic redshifts from Gemini identified on an SDSS r-band image. Blue boxes (red circles) denote members with higher (lower) redshifts than the systemic cluster redshift of z = 0.363. Large, bold symbols mark the BCGs of both kinematic components. The 148 GHz Compton y SZ contours are superposed. The contours start at a level of 2.0 × 10 −5 , increasing towards the centre in steps of 1.25 × 10 −5. The black X marks the cluster SZ peak.

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Article
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We present the detection of a giant radio halo (GRH) in the Sunyaev-Zel'dovich (SZ)-selected merging galaxy cluster ACT-CL J0256.5+0006 (z = 0.363), observed with the Giant Metrewave Radio Telescope at 325 MHz and 610 MHz. We find this cluster to host a faint (S610 = 5.6 ± 1.4 mJy) radio halo with an angular extent of 2.6 arcmin, corresponding to 0...

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... this red- shift information, we can estimate an independent dynami- cal mass and re-examine the merger geometry proposed by M04 (see Section 5.2 below). The cluster members are shown in Figure 1 where red circles (blue boxes) denote members that are at lower (higher) redshifts than the cluster redshift of z = 0.363. We identify these two sets of galaxies as sep- arate kinematic components (see Section 5.2 below), each of which has a brightest cluster galaxy (BCG) that is indi- cated by a large, bold symbol. ...
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... there are two BCGs (cluster members with the lowest SDSS magnitudes) that are spatially separated, as seen from the SDSS image in Figure 1, which are also sepa- rated in velocity space as shown in Figure 9. This provides support for the existence of two distinct galaxy populations. ...
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... simplicity, we assume the same merger geometry as in M04, schematically outlined in Figure 10. Working in the rest frame of the main component, we assume the same simplification of a point mass subcluster and ignore dynamical friction. ...
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... implies that the impact angle must be less than 90 • . Using simple trigonometry, it follows from the merger geom- etry in Figure 10 that dmin d ...
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... solving equations 8 and 9 with these constraints provides two sets of solutions for the merger model. These are listed in Table 9, with the graphical so- lutions given in Figures 11 and 12. The uncertainties on v, d, and θ are shown in Figures 11 (v and d) and 12 (d and θ), and are propagated from the uncertainties on the R200 mass and radius of the main cluster component, the R200 radius of the subcluster, and measured line-of-sight velocity difference. ...
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... estimate the merger time-scales for J0256 we assume a simple merger taking place in a linear fashion along the merger axis determined by the impact angle, θ, schemati- cally outlined in Figure 13. In Section 2.1, we ruled out a scenario in which the subcluster has already passed through the core. ...
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... Section 2.1, we ruled out a scenario in which the subcluster has already passed through the core. In Figure 13, we isolate three distinct times during the merger: (A) first virial crossing; (B) core passage; and (C) second virial crossing. Even though we refer to virial crossing, we use R200 as a proxy for the virial radius. ...
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... case 1, J0256 is closer to the be- ginning of its merger with ∼460 Myr until first core passage. Figure 13. Schematic showing the relative position of the subcluster (red circles) to the main cluster (black circle) overlaid on the X-ray image at three different times during the merger: (A) first virial crossing; (B) core passage; and (C) second virial crossing. ...

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... The upper limit to the spectral index implied by our ASKAP and ATCA maps is also far steeper than the typical spectral index of many radio haloes (e.g. Dallacasa et al. 2009 ;Knowles et al. 2016 ;Shweta, Athreya & Sekhar 2020 ;Wilber et al. 2020 ;Bruno et al. 2021 ;Duchesne et al. 2021b,d ;Rajpurohit et al. 2021a , b ). Thus, the nature of this source is not immediately obvious. ...
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... All statistical, uniformly-selected cluster samples used in radio halo studies have to date been restricted to high masses (M 500 6 × 10 14 M ) and lower redshift ranges ( 0.1 z < 0.4; e.g., Venturi et al. 2007;Cuciti et al. 2015), with current turbulent reaccleration formation theories predicting a sharp drop in the occurence of radio halos at higher redshift, where cluster magnetic fields are expected to be weaker (Cassano et al. 2006;Brunetti & Jones 2014). Diffuse emission has also been detected in some lowmass (e.g., Knowles et al. 2016b;Bernardi et al. 2016;Kale et al. 2017;Hlavacek-Larrondo et al. 2018;Brüggen et al. 2018;Hoang et al. 2020) and high-redshift (z > 0.5; Bonafede et al. 2009;Lindner et al. 2014;Pandey-Pommier et al. 2013;Riseley et al. 2017;Knowles et al. 2019;Giovannini et al. 2020) systems. Most of these detections result from single-target programmes or small samples. ...
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