A spatially resolved study of ionized regions in galaxies at different ...

A spatially resolved study of ionized regions in galaxies at different ... A spatially resolved study of ionized regions in galaxies at different ...

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38 2 • The star formation history of NGC 5471 region. In order to visualize this, we have selected four different areas in the CMD and proceeded to locate spatially the stars in these four boxes. Figure 2.11 displays the resulting distributions. The youngest and more massive stars (a) are clearly concentrated in the main star forming emission line knots, implying that massive stars form mainly in clusters. Only two stars are not directly associated with these knots, one of which belongs to an isochrone of 20 Myr. Panel (d) displays the distribution of intermediate mass stars (∼ 5−10 M ⊙ ) older than about 50 Myr; these stars are distributed mainly towards the halo, with only a few in the core of the region. Panels (b) and (c) show the distribution of intermediate mass stars (∼ 10 − 15 M ⊙ ), both those which are in the main sequence and those which have already evolved out of it. The distributions of stars in these two CMD boxes are clearly fairly uniform throughout the core of NGC 5471, with some of them distributed in the halo, a somewhat complementary spatial distribution to the older lower mass stars in the bottom-right panel. Because the stars in these two intermediate boxes are of the same mass but they are found in a range of evolutionary stages, this implies that star formation has proceeded more or less uniformly in the core for the last ∼ 20 − 50 Myr. From this analysis of the spatial distribution of the CMD, a clear picture emerges in which the star formation in the NGC 5471 complex has proceeded in a general spatiotemporal sequence from the halo inwards to the core. During the first epoch, ∼ 50−100 Myr ago, the star formation occurred mainly in the halo, then it moved inwards and occurred more or less uniformly in the core ∼ 20 − 50 Myr ago, although some of the star formation was also important in the halo, and finally the current ionizing star forming event is mostly concentrated in the singular bright clusters well located within the core. At the same time, we have seen that, both from the integrated photometric analysis and from the CMD, as the events moved inwards from the halo to the core the amount of mass of gas formed into stars seems to have increased. We note that the current event of ionizing clusters is apparently contained within a large bubble which defines the core of NGC 5471. This bubble, of projected size 400 × 550 pc, is clearly defined geometrically (cf. Figure 2.2) and kinematically (Munoz-Tunon et al., 1995), and is likely to have been produced by the stars that formed ∼ 20 Myr ago. There are other examples that seem to follow the general process of star formation that we have outlined here for NGC 5471. Walborn and Blades (1997) find a similar spatio-temporal distribution of stars in 30 Doradus, and Úbeda et al. (2007) also find an inwards sequence of star formation and a bubble for cluster I-A in NGC 4214.

Chapter 3 Integral Field Spectroscopy of Hii region complexes. The outer disk of NGC 6946 3.1 Introduction NGC 6946 is a relatively nearby, nearly face–on spiral galaxy with an exceptionally gas–rich disk which shows evidence for a high star formation rate (SFR) throughout (Degioia-Eastwood et al., 1984) and has been classified as having strong nuclear starburst activity (Elmegreen et al., 1998). The six historical supernova remnants recorded during the past century attest to this high star formation and justify the popular name “Fireworks Galaxy”. NGC 6946’s orientation and large angular size (D 25,B = 11. ′ 2) offers the prospect of studying the structure and star forming properties of the disk. NGC 6946 and its many supernova remnants have been the subject of numerous X–ray, optical and radio papers. At mm wavelengths the CO molecule, used as a tracer of the dominant molecular species, H 2 , has been observed by several authors (Ball et al., 1985; Casoli et al., 1990), showing that the CO distribution has a central density peak and barlike gas structure. Morphologically, NGC 6946 is a late-type SAB(rs)cd spiral galaxy (de Vaucouleurs et al., 1991), with several spiral arms and star-forming regions scattered throughout the disk, considerable extinction and a small nucleus. Its general properties are summarized in Table 3.1. K-band images reveal four prominent, not very symmetric arms (Regan and Vogel, 1995). 39

38 2 • The star form<strong>at</strong>ion history <strong>of</strong> NGC 5471<br />

region. In order to visualize this, we have selected four <strong>different</strong> areas <strong>in</strong> the CMD and<br />

proceeded to loc<strong>at</strong>e <strong>sp<strong>at</strong>ially</strong> the stars <strong>in</strong> these four boxes. Figure 2.11 displays the result<strong>in</strong>g<br />

distributions. The youngest and more massive stars (a) are clearly concentr<strong>at</strong>ed <strong>in</strong> the ma<strong>in</strong><br />

star form<strong>in</strong>g emission l<strong>in</strong>e knots, imply<strong>in</strong>g th<strong>at</strong> massive stars form ma<strong>in</strong>ly <strong>in</strong> clusters. Only<br />

two stars are not directly associ<strong>at</strong>ed with these knots, one <strong>of</strong> which belongs to an isochrone<br />

<strong>of</strong> 20 Myr. Panel (d) displays the distribution <strong>of</strong> <strong>in</strong>termedi<strong>at</strong>e mass stars (∼ 5−10 M ⊙ ) older<br />

than about 50 Myr; these stars are distributed ma<strong>in</strong>ly towards the halo, with only a few <strong>in</strong><br />

the core <strong>of</strong> the region. Panels (b) and (c) show the distribution <strong>of</strong> <strong>in</strong>termedi<strong>at</strong>e mass stars<br />

(∼ 10 − 15 M ⊙ ), both those which are <strong>in</strong> the ma<strong>in</strong> sequence and those which have already<br />

evolved out <strong>of</strong> it. The distributions <strong>of</strong> stars <strong>in</strong> these two CMD boxes are clearly fairly uniform<br />

throughout the core <strong>of</strong> NGC 5471, with some <strong>of</strong> them distributed <strong>in</strong> the halo, a somewh<strong>at</strong><br />

complementary sp<strong>at</strong>ial distribution to the older lower mass stars <strong>in</strong> the bottom-right panel.<br />

Because the stars <strong>in</strong> these two <strong>in</strong>termedi<strong>at</strong>e boxes are <strong>of</strong> the same mass but they are found<br />

<strong>in</strong> a range <strong>of</strong> evolutionary stages, this implies th<strong>at</strong> star form<strong>at</strong>ion has proceeded more or less<br />

uniformly <strong>in</strong> the core for the last ∼ 20 − 50 Myr.<br />

From this analysis <strong>of</strong> the sp<strong>at</strong>ial distribution <strong>of</strong> the CMD, a clear picture emerges <strong>in</strong><br />

which the star form<strong>at</strong>ion <strong>in</strong> the NGC 5471 complex has proceeded <strong>in</strong> a general sp<strong>at</strong>iotemporal<br />

sequence from the halo <strong>in</strong>wards to the core. Dur<strong>in</strong>g the first epoch, ∼ 50−100 Myr<br />

ago, the star form<strong>at</strong>ion occurred ma<strong>in</strong>ly <strong>in</strong> the halo, then it moved <strong>in</strong>wards and occurred<br />

more or less uniformly <strong>in</strong> the core ∼ 20 − 50 Myr ago, although some <strong>of</strong> the star form<strong>at</strong>ion<br />

was also important <strong>in</strong> the halo, and f<strong>in</strong>ally the current ioniz<strong>in</strong>g star form<strong>in</strong>g event is mostly<br />

concentr<strong>at</strong>ed <strong>in</strong> the s<strong>in</strong>gular bright clusters well loc<strong>at</strong>ed with<strong>in</strong> the core. At the same time,<br />

we have seen th<strong>at</strong>, both from the <strong>in</strong>tegr<strong>at</strong>ed photometric analysis and from the CMD, as the<br />

events moved <strong>in</strong>wards from the halo to the core the amount <strong>of</strong> mass <strong>of</strong> gas formed <strong>in</strong>to stars<br />

seems to have <strong>in</strong>creased.<br />

We note th<strong>at</strong> the current event <strong>of</strong> ioniz<strong>in</strong>g clusters is apparently conta<strong>in</strong>ed with<strong>in</strong> a large<br />

bubble which def<strong>in</strong>es the core <strong>of</strong> NGC 5471. This bubble, <strong>of</strong> projected size 400 × 550 pc, is<br />

clearly def<strong>in</strong>ed geometrically (cf. Figure 2.2) and k<strong>in</strong>em<strong>at</strong>ically (Munoz-Tunon et al., 1995),<br />

and is likely to have been produced by the stars th<strong>at</strong> formed ∼ 20 Myr ago.<br />

There are other examples th<strong>at</strong> seem to follow the general process <strong>of</strong> star form<strong>at</strong>ion th<strong>at</strong> we<br />

have outl<strong>in</strong>ed here for NGC 5471. Walborn and Blades (1997) f<strong>in</strong>d a similar sp<strong>at</strong>io-temporal<br />

distribution <strong>of</strong> stars <strong>in</strong> 30 Doradus, and Úbeda et al. (2007) also f<strong>in</strong>d an <strong>in</strong>wards sequence<br />

<strong>of</strong> star form<strong>at</strong>ion and a bubble for cluster I-A <strong>in</strong> NGC 4214.

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