EDP Sciences
Free Access
Issue
A&A
Volume 606, October 2017
Article Number A131
Number of page(s) 3
Section Extragalactic astronomy
DOI https://doi.org/10.1051/0004-6361/201731372
Published online 24 October 2017

© ESO, 2017

1. Introduction

A 1.5 deg2 region of the nearby cluster of galaxies Abell 1367 (z ~ 0.0217) was recently surveyed with deep Hα observations using the Subaru telescope (Yagi et al. 2017). These observations, at the limiting surface brightness of 2.5 × 10-18 erg cm-2 s-1 arcsec-2, revealed the presence of Hα tails behind ten out of the cluster’s 26 late-type galaxies (LTG) that were surveyed. This indicates that, when observed with sufficiently deep observations, approximately 40% of all LTGs in this cluster reveal an associated extended trail of Hα, in agreement with the frequency obtained in the Coma cluster by Yagi et al. (2010). This evidence strengthens previous suggestions that a massive infall of gas-rich, star forming galaxies (100–400 galaxies per Gyr, Adami et al. 2005; Boselli et al. 2008; Gavazzi et al. 2012, 2013a,b) is occurring at the present epoch onto rich clusters of galaxies such as Coma and Virgo. This estimate derives from the combined evidence that ionized tails arise from the ram pressure stripping (Gunn & Gott 1972) of galaxies crossing the intracluster medium at high speed for the first time, and that the gas ablation produced by such interaction proceeds on timescales as short as 100 Myr (Boselli & Gavazzi 2006, 2014).

thumbnail Fig. 1

Gray-scale representation of the Hα emission from CGCG 97-121 (left) and 2MASX J11443212+2006238 (right), with levels chosen to highlight the bright part of the emission. Smoothed (by 2.8 arcsec) contours of the Hα-NET image show the low-brightness, extended tail behind 2MASX J11443212+2006238 whose maximum projected length is 85 kpc. North is at the top and east to the left.

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Table 1

Observational parameters of the two target galaxies.

The galaxy 2MASX J11443212+2006238 lies very close to the edge of the Subaru field (see Fig. 9 of Yagi et al. 2017), preventing a robust measurement of the extended Hα flux and of its total length. Guided by these observations, we decided to devote two entire (moon free, clear but not photometric) nights of observations at the 2.1 m telescope of the San Pedro Martir observatory to the field containing 2MASX J11443212+2006238 and another cluster member: CGCG 97-121 (Zwicky et al. 1961–68). In spite of the three-times-shallower data obtained with our smaller telescope, we could detect the full extent of the Hα emission trailing behind 2MASX J11443212+2006238.

2. Observations

On the nights of April 24 and 25, 2017, we used the 2.1 m telescope at San Pedro Martir to repeatedly observe a 5 × 5 arcmin2 region of the nearby cluster of galaxies Abell 1367. We used a narrow (80 Å) band filter centered at 6723 Å to detect the Hα emission (at the mean redshift z ~ 0.0217 of the cluster) and a broad band r (Gunn) filter (effective λ 6231 Å, Δλ ~ 1200 Å) to recover the continuum emission.

The field, which contains both 2MASX J11443212+ 2006238 and CGCG 97-121, was observed with 33 independent pointings of 900 s with the ON-band filter, and with 25 pointings of 180 s with the broad band (OFF-band) r filter. After flat-fielding, the aligned observations were combined into a final ON-band frame totalling 8.25 h exposure, and an OFF-band frame of 1.25 h exposure (details on the reduction procedures of Hα observations can be found in Gavazzi et al. 2012). To calibrate the data, which were observed in clear sky conditions, we used the Sloan Digital Sky Survey (SDSS) nuclear fiber spectrum of 2MASX J11443212+2006238 from which we measure an Hα point-like flux (within the central 3 arcsec) of 2.45 × 10-14erg cm-2 s-1 Å-1. Assuming this flux within the 3′′ central aperture of the galaxy, we derive an effective zero point for our observations of –15.29 erg cm-2 s-1 this should be compared with –15.54 obtained in the previous photometric nights and we estimate a limiting surface brightness at Hα ≈ 7.9 × 10-18 erg cm-2 s-1 arcsec-2.

3. Results

In Table 1 we list the celestial coordinates, redshift, total stellar mass, and total equivalent width (EW) and flux separately for 2MASX J11443212+2006238, for the diffuse trailing material, and for CGCG 97-121. The flux of the diffuse gas of 2MASX J11443212+20062 (in parenthesis) is measured in a polygonal aperture that fits the last contour level shown in Fig. 1. Stellar masses were derived from the i-band luminosity and the gi color according to Zibetti et al. (2009), assuming a Chabrier initial mass function (IMF; Chabrier 2003). Figure 1 shows the continuum subtracted Hα image of our field smoothed by 2.8 arcsec, from which we measured the extent of the diffuse flux associated to 2MASX J11443212+2006238. Assuming a distance from Abell 1367 of 95 Mpc, the tail extends in the NE direction for 85 kpc. Such a distance can be covered in 85 Myr by a galaxy travelling at approximately 1000 km s-1, which is the typical velocity of galaxies in clusters. Given that this length is typical in Abell 1367 (the tail length ranges from 15 to 230 kpc in this cluster, Yagi et al. 2017), 85–100 Myr can be assumed as the typical time during which the tails remain visible. This time is longer than the typical electron recombination time, recently estimated as 0.2 Myr for UGC 6697 (Consolandi et al. 2017) and even shorter for ESO137-001 (Fossati et al. 2016), suggesting the existence of some mechanism capable of keeping the gas ionized for a longer period of time in the wakes of the extended tails. However, 100 Myr is a rather short period of time in cosmic history. This suggests that the ram pressure stripping phenomenon occurs during the first pericenter passage over a short period of time, consistent with the evidence of truncated star formation at the southern side (opposite to the tail) of 2MASX J11443212+20062 (Yagi et al. 2017), which could indicate quenching timescales as short as 100 Myr (see Boselli et al. 2006, 2016a,b). The very existence of 11 tails of similar typical length allows us to roughly estimate the infall rate of galaxies in A1367 as 130 per Gyr, consistent with other existing estimates for Coma and Virgo.

Acknowledgments

This research has made use of the GOLDmine database (Gavazzi et al. 2003, 2014b) and of the NASA/IPAC Extragalactic Database (NED), which is operated by the Jet Propulsion Laboratory, California Institute of Technology, under contract with the National Aeronautics and Space Administration.

References

All Tables

Table 1

Observational parameters of the two target galaxies.

All Figures

thumbnail Fig. 1

Gray-scale representation of the Hα emission from CGCG 97-121 (left) and 2MASX J11443212+2006238 (right), with levels chosen to highlight the bright part of the emission. Smoothed (by 2.8 arcsec) contours of the Hα-NET image show the low-brightness, extended tail behind 2MASX J11443212+2006238 whose maximum projected length is 85 kpc. North is at the top and east to the left.

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