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

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68 3 • IFS <strong>of</strong> a GEHR <strong>in</strong> NGC 6946<br />

Cre<strong>at</strong><strong>in</strong>g maps<br />

Maps are d<strong>at</strong>a files stored <strong>in</strong> 2D fits files, reflect<strong>in</strong>g the orig<strong>in</strong>al arrangement <strong>of</strong> the spaxels<br />

<strong>in</strong> the sky. In the case <strong>of</strong> non regularly gridded IFU or RSS files, it is necessary to <strong>in</strong>terpol<strong>at</strong>e<br />

the d<strong>at</strong>a, as mentioned <strong>in</strong> previous sections. We have used <strong>in</strong>terpol rout<strong>in</strong>e from E3D with<br />

a nearest neighbour <strong>in</strong>terpol<strong>at</strong>ion, a grid parameter 13 <strong>of</strong> 10 −12 and a pixel size <strong>of</strong> 1 ′′ , close to<br />

the recommended 1/3 <strong>of</strong> the orig<strong>in</strong>al spaxel size. All the maps shown <strong>in</strong> next sections, unless<br />

mentioned, have a North down and East left orient<strong>at</strong>ion, and a 1 ′′ /pixel scale. A distance <strong>of</strong><br />

5.9 Mpc to NGC 6946 is assumed, so 1 ′′ <strong>in</strong> the sky corresponds to 28.6 pc.<br />

We have masked all values <strong>in</strong> the maps with rel<strong>at</strong>ive errors ≥ 25%. This is applied to<br />

any quantity: flux, r<strong>at</strong>io or comb<strong>in</strong><strong>at</strong>ion <strong>of</strong> l<strong>in</strong>es used <strong>in</strong> empirical parameters.<br />

3.4.3 Hα maps and morphology<br />

From Figure 3.14 it is clear th<strong>at</strong> the morphology <strong>of</strong> the complex <strong>of</strong> Hii <strong>regions</strong> is well<br />

recovered from the IFU d<strong>at</strong>a. The upper panel is an Hα flux map cre<strong>at</strong>ed from the RSS<br />

blue d<strong>at</strong>a as expla<strong>in</strong>ed <strong>in</strong> section 3.4.2. The masked values follow the criteria expla<strong>in</strong>ed <strong>in</strong><br />

th<strong>at</strong> section, as well as the orient<strong>at</strong>ion (north down, east left). The lower panel shows an Hα<br />

(not cont<strong>in</strong>uum-subtracted) image taken <strong>at</strong> the Kitt Peak N<strong>at</strong>ional Observ<strong>at</strong>ory (KPNO)<br />

2.1-meter telescope (same source as Figure 3.3) show<strong>in</strong>g the PPak field and with the same<br />

orient<strong>at</strong>ion as the map <strong>of</strong> the upper panel.<br />

Hodge and Kennicutt (1983) c<strong>at</strong>alogued more than 10000 Hii <strong>regions</strong> <strong>in</strong> 125 <strong>galaxies</strong>.<br />

This HK c<strong>at</strong>alog conta<strong>in</strong>s 540 identified Hii <strong>regions</strong> <strong>in</strong> NGC 6946. We have labelled all the<br />

important knots follow<strong>in</strong>g the HK identific<strong>at</strong>ion. As it can be seen <strong>in</strong> the Hα map, only the<br />

most <strong>in</strong>tense knots are clearly def<strong>in</strong>ed, and for this reason we have labelled them with the<br />

first four alphabetical letters. Interest<strong>in</strong>gly, knot B is not identified <strong>in</strong> Hodge and Kennicutt<br />

(1983). S<strong>in</strong>ce they have enough signal-to-noise, we will present the ma<strong>in</strong> measured properties<br />

<strong>of</strong> these four knots when discuss<strong>in</strong>g the <strong>in</strong>tegr<strong>at</strong>ed properties <strong>in</strong> section 3.4.8. It has to be<br />

remarked th<strong>at</strong> the lower panel image has not been cont<strong>in</strong>uum-subtracted, so some knots are<br />

seen more <strong>in</strong>tense s<strong>in</strong>ce their cont<strong>in</strong>uum sources are <strong>in</strong>cluded <strong>in</strong> the image, but their Hα<br />

emission are not so strong. This is the case <strong>of</strong> knots HK83-013, HK83-014, HK83-009 and<br />

HK83-006.<br />

Figure 3.15 shows the cont<strong>in</strong>uum emission near Hα (top) and Hβ (bottom) maps together<br />

with the correspond<strong>in</strong>g emission l<strong>in</strong>e <strong>in</strong>tensity isocontours overplotted, while Figure<br />

3.16 shows the cont<strong>in</strong>uum emission map near 8500 Å together with the Hα isocontours overplotted<br />

as reference. The red cont<strong>in</strong>uum comes from the first po<strong>in</strong>t<strong>in</strong>g. Maps <strong>of</strong> the cont<strong>in</strong>ua<br />

are represent<strong>at</strong>ive <strong>of</strong> the stellar emission, free <strong>of</strong> contam<strong>in</strong><strong>at</strong>ion from the gaseous emission<br />

l<strong>in</strong>es. From the Hα and Hβ isocontours it can be seen th<strong>at</strong> both emission structures are<br />

13 The grid parameter represents the resolution <strong>of</strong> the triangul<strong>at</strong>ion.

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