<<

Broadband Colors

1 15 02 00 IC 3392 IC 3392 IC 3392 01 30

00

00 30 Ηα NaD

00 Ηβ Mgb 14 59 30 Declination (J2000) Ηγ 00 Ηδ

58 30

00 1’

12 28 52 50 48 46 44 42 40 38 36 34 Right Ascension (J2000) 4.5 kpc

NGC 4569 NGC 4569 NGC 4569 13 14

12 NaD Ηα 10 Ηβ Mgb Ηγ Declination (J2000) Ηδ 08

06 1’ 04 12 37 10 05 00 36 55 50 45 40 35 30 Right Ascension (J2000) 4.5 kpc 09 13 00 NGC 4522 12 30 NGC 4522 NGC 4522

00

11 30

00

10 30 Mgb 00 NaD Declination (J2000) Ηδ 09 30 Ηβ Ηγ Ηα 00

08 30

00 1’ 12 33 50 45 40 35 30 Right Ascension (J2000) 4.5 kpc

2 Color Magnitude Diagrams

NGC 4580 NGC 4064 IC 3392 t q > 400 Myr NGC 4405 NGC 4388 NGC 4569

NGC 4424 t q = 200 − 350 Myr

NGC 4522 t q < 100 Myr

3 Cortese & Hughes (2009) 4 L. Cortese & T.M. Hughes

HI-normal late types occupy the blue cloud, but HI-deficient tend to scatter everywhere

Figure 1. The NUV − H colour-stellar-mass relations for our sample. Colours are corrected for internal and Galactic extinction, 8 L. Cortese & T.M. Hughesas described in § 2.1. Late and early-types are indicated with circles and squares respectively. The separation between blue and red sequence is clearly evident in the right panel where only Hi-normal late-type galaxies are shown. The dotted lines in both panels show the boundaries of the transition region as defined in § 3. Typical errors, including the uncertainty in the extinction6 correction,L. Cortese are shown. & T.M. Hughes outflow has been interpreted as related to bar instability and it is not clear whether such process can be responsible for i the H deficiency observed in this object. Thus, the origin of our colour-cut must be considered as a conservative upper- i the H deficiency in these two objects still remains unclear. limit in the case of dwarf systems. On the other side, UV-to-near-infrared colours typical 5.1.1 Time-scales for the migration of the red sequence (NUV H !6) can either indicate − low residual formation activity or old, evolved stellar Combining the observational evidence presented above with populations (e.g. Boselli et al. 2005b). The phenomenon of previous works on the cluster (e.g. Boselli & Gavazzi the UV-upturn (O’Connell 1999) makes colours redder than 2006 and references therein), we favor hydrodynamical in- NUV H 6difficult to interpret so that the NUV H − ∼ − teractions like ram-pressure as the main process responsible colour cannot be considered anymore as a good proxy for the for the suppression of the . However, we note specific star formation rate (SSFR). Following Kaviraj et al. that gravitational interactions cannot be excluded in at least (2007), we use observations of well knownFigure strong 4. The UV-upturn link between Hi-content and colour. Left: NUV − H colour vs. Hi deficiency. The vertical dotted line separates galaxies with ‘normal’ gas content from Hi-deficient systems. Center: NUV − H colour vs. gas-fraction. Right: FUV − H vs. gas-fraction. Late- one case (NGC4438, e.g., Kenney et al.Figure 2008; 2. BoselliThe morphological et al. type distribution of galaxies in our galaxies to derive a lower limit on the NUV H colour i and early- type− galaxies are indicated with circles and squares respectively. Empty symbols highlight detected H -deficient galaxies, while 2005a; Vollmer et al. 2005a). sample (dotted histogram). The filled histogram represents galax- typical of evolved stellar populations.arrows In details, show upper given limits. t Thehe horizontal dashed-lines show the boundaries of the transition region, as defined in § 3. Only recently, has it become possibleies in the to transition accurately region, while red and blue sequence galaxies typical colour observed in M87 (NUV H 6.1 mag) and are shown with the empty and dashed histogram, respectively. − ∼ quantify the time-scale for the quenching of the star Figure 7. Same as Fig. 1 (left panel).NGC4552 Large symbols (NUV indicatesH 6.4 mag), we assumedtered1.Thissuggeststhat,forNUV H=6 NUV H>4.5 mag, the − ∼ − − formation after the stripping event (Boselli et al. 2006; galaxies in the Crowl & Kenney (2008)mag sample as for a conservative which a strip- lower limit to discriminategas-fraction is not between a goodHI-deficiency proxy of the UV-optical colourcorrelates with color ping time-scale estimate is available. Stripping time-scale shorter anymore and vice-versa. The dispersion in the colour-gas- Crowl & Kenney 2008). Luckily, almost all the objects for residual star formation and UV-upturn.fraction Thevalidity relation increases of this from 0.35 dex (consistent with ∼ which a stripping time-scale has been computed are included than 300 Myr and between 300-500 Myrcolour-cut are shown with is confirmed hexagons by a visual inspectionKannappan 2004 of GALEX and Zhang et al. 2009) to 0.54 dex when which do not belong either to the blue cloud or the red i ∼ in our sample. In Fig. 7, we highlight the position of these six and triangles respectively. colour images, which indicates that onlywe 6% move (i.e. from 6 H objects)-normal blue-cloud galaxies to transition sequence. and red-sequence objects. This is in reality a lower-limit on objects in the colour-mass diagram according to the age of of galaxies redder than NUV H=6 mag show clear evi- On one side, it is difficult to determine (both obser- − the real scatter increase since upper-limits are not included the stripping event: hexagons and triangles indicate galax- dence of residual SF (e.g., blue star-formingin the calculation. knots). vationally and theoretically) where the blue cloud ends. In ies in which the star formation in the outer regions has been tionUsing (Cowie our & Songaila own 1977), results may thus playagainst an important us The results shown in Fig. 4 are strongly suggestive of this paper we decide to use the blue cloud of Hi-normal The morphological type distributionsa) a diff forerent galaxies evolutionary be- path followed by Hi-deficient and suppressed less or more than 300 Myr, respectively. Inter- role in the complete suppression of the star formation. i galaxies to determine the range of colours typical of unper- longing to the three groups here consideredH -normal (i.e., galaxies blue outside cloud, the blue cloud and b) of a weaker ∼ An upper limit to the time spent by Hi-deficient galax- link between Hi-content and colour than the one typically estingly, there is a difference in the average colour between red sequence and transition region) are shown in Fig. 2. It Figure 5. The stellar mass distribution of transition galaxies turbed galaxies. This is motivated by the fact, discussed in observed in star-forming galaxies. Therefore, in order to gain 4 ies in the transition region can be obtained if we assume that (filled circles). Left: Spirals (empty squares), lenticulars (trian- very recent quenching (t<300 Myr) and older events, so that i clearly emerges that red and blue galaxiesadditional are insights two disjoint on the evolution of galaxies in the tran- HC09, that the transition regionall the is mainly remaining populated gas will by be H consumed- by star formation. It gles) and E+dE (asterisks) are indicated. Right: Galaxies are only galaxies with quenching time-scale 400-500 Myr are families not only in colour, but also insition shape. region, in the following we divide transition galaxies i deficient∼ galaxies in high-density environments. Hi-normal highlighted according to their H content. Galaxies for which the at the edge or have already reached the transition region. is in fact plausible that the intra-cluster medium will pre- into two families according to their gas content and investi- estimate of Hi deficiency is unsure are indicated with asterisks. late-type galaxies form a bluevent cloud additional clearly separated infall of cold from gas. In thisOf case, course, the ‘Robert the criterias’ described abovegate separatelyare arbitrary their properties. and This is consistent with the fact thatthe the red Virgo sequence transition at all masses, as shown in the right panel of vary according to the colour adopted and toBefore the investigating stellar mass the detailed properties of transition time’ (Roberts 1963, defined as the ratio of the gas mass 5THEPROPERTIESOFTRANSITION population is not virialized, implyingFig. 1. aWe recent thus ( define1.7 galaxies with suppressed star forma- range investigated. This can be clearlygalaxies, seen in it Fig. is worth 3, where adding a few notes about the validity of ≤ to the current star formation rate: i.e., M(gas)/SFR) can the classification for Hi-normal transition systems. The low GALAXIES Gyr, i.e., the Virgo crossing time; Bosellition as & those Gavazzi objects 2006) with NUV H>4.5 mag (correspond- the position of ‘transition galaxies’ in different UV and op- number of objects in this category and the large uncertain- In total, 67 galaxies in our sample, corresponding to 17% infall into the cluster center. Thus, we can conclude that be used− to obtain a rough estimate of the gas consumption ∼ ing to the 90th percentile of the colour of Hi-normal spi- tical colour-stellar-mass diagrams is highlighted.ties in the estimate Altho of gasugh fractions and UV dust attenuation in both number and total stellar-mass lie in the transition once the Hi has been stripped from the disk, a galaxy moves10 time. Assuming that 15% of the total gas is in the molecular might suggest that these are just random outliers, not differ- region as defined in 3. In Fig. 5, we show the stellar- rals with Mstar >10 M!), consistently with Martin et al. it is indisputable that not all transition galaxies are outsidei § from the blue cloud to the transition region in a time-scale state (Boselli et al. 2002) and 30% is composed by helium ent from the bulk of the H -deficient population. Although mass distribution of transition galaxies divided accordingto (2007a). This colour-cut roughly corresponds to star forma-∼ the red sequence in a FUV H and NUVwe cannot excludeB colour the presence di- of a few misclassified galax- and heavy elements (Boselli et al. 2001), we find that the − − their morphological type (left panel) and gas content (right roughly 0.5-1 Gyr. ies in both the Hi-deficient and Hi-normal population, it is 10 tion histories (SFHs) having e-folding time-scale of 3Gyr agram3 (in particular at low stellar-masses), it emerges that panel). For M∗ ! 10 M",galaxieswith4.5

No. 6, 2009 VIVA. I. 1753

Figure 8. Examples of the different H i morphologies found in the survey. Total H i images are shown in white contours overlaid on the SDSS images. The thick white bar in the bottom-left corner indicates 1 arcmin in each panel. The top row shows examples of gas-rich galaxies in gas rich environments in the outskirts, the middle row shows galaxies at intermediate distances, while the bottom row shows examples of severely truncated H i disks at a range of projected distances from M87. 5

(2004)arguethatthemergingofthesubclusterM49withVirgo 7. SUMMARY could locally enhance the due to bulk motions, clumpy density distributions, and variations in the temperature We present the results of a new H i imaging survey of 53 of the ICM gas. A temperature map of the X-ray emission galaxies in the . The goal is to study the impact of (Shibata et al. 2001)doesshowthatNGC4522islocated different environmental effects on the H i disks of the galaxies. near strong variations in the X-ray temperature. The results Virgo is ideal for this type of study as it is dynamically young on galaxies such as NGC 4064 and NGC 4522 fit in nicely with and potentially contains galaxies that are affected by a wide recent work by Tonnesen et al. (2007)andTonnesen&Bryan range of environmental effects. Its nearness allows us to study (2008), who find that ram pressure can vary by more than a the individual galaxies in great detail. factor of 10 at a given distance from the cluster center due to the We have selected 48 galaxies and obtained data on five structure in the ICM. This makes it possible for some galaxies to additional galaxies that were in the same field and velocity range get stripped in the outskirts without ever making it to the center as the target galaxies. The galaxies were selected to cover a wide of the cluster, something that we may be witnessing in Virgo. range of star formation properties, from anemic to starburst, and

0.1 (g-r)

DHI/DB DHI/DK

6

0.1 (g-r)

DHI/DB DHI/DK

7 Hogg et al (2004)

High density environments (δ1x8 > 7.0) All Sersic values

8 Questions/Thoughts

•What is the story of the paper? • Galaxies with large HI disks are blue; those with small HI disks are red • Galaxies that were stripped very recently occupy the blue cloud, those stripped longer ago occupy the green valley, and those stripped longest ago occupy the red sequence • It seems that it takes ~500 Myr to transform from blue to red. • Galaxies with disturbed HI disks have very recent star formation and blue colors; those with undisturbed disks have less recent star formation.

•How are we different from Cortese & Hughes (2009)? • We know HI morphologies • We know (or think we know) what happened to a lot of these galaxies

•What should we do about the fact that we are comparing cluster galaxies to all galaxies? • I think this comparison is important, but it would ALSO be great to compare our sample to a larger “cluster-like” sample. • Is it possible to get Blanton (2003)’s CMD with the environment data that Hogg et al. (2004) has for the brightest galaxies? • How important is this comparison to this paper?

9 Questions/Thoughts

• Many things different things may have happened to the Virgo Cluster galaxies (RPS, mergers, harassment, starvation (?), etc.) • We only have timescales for the RPS galaxies; how much can we say about general timescales based on only the RPS results? • Is it reasonable to acknowledge that there are many things that happen and then focus on the RPS timescale results •Other things?

10