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 ...
70 3 • IFS of a GEHR in NGC 6946 60¡DEC (arcsec) 50 40 30 20 10 0 0 10 20 30 40 50 60 70 RA (arcsec) 60¡DEC (arcsec) 50 40 30 20 10 0 0 10 20 30 40 50 60 70 RA (arcsec) Figure 3.15: Maps in the continuum near Hα (top) and Hβ (bottom) emission lines together with the isocontours of the corresponding emission line flux overplotted. Maps are displayed in linear scale, while isocontours are in logarithmic scale. Contours are masked according to their emission line flux.
3.4. Results 71 60¡DEC (arcsec) 50 40 30 20 10 0 0 10 20 30 40 50 60 70 RA (arcsec) Figure 3.16: Maps in the continuum near 8500 Å together with the isocontours of Hα overplotted. Map displayed in linear scale, while the isocontour in logarithmic scale. Contours are masked accordingly to their emission line flux. The continuum map source comes from the (red) first pointing. quite similar, with the four main intense knots (A, B, C and, D) well demarcated. The brightest knot, A, has the most extended structure, with a tail pointing to the north-west. This structure seems to be formed following the continua morphology. There are not many differences between the continuum maps of Hα and Hβ. The peak intensity of the continuum in knot A corresponds to the same position in both emission line maps. From the continuum emission, it can be seen that the structure of knot A defines that of the Hα map, with a small concentration to the west of the knot, probably being the source of the north-west tail of this knot. Although the rest of knots have their equivalence between their emission line maps and continua, their maximum position are not the same. A remarkable structure is the one of knot C, which has an elongated continuum in a south-east to north-west direction, while the emission line morphology is egg-like (ellipsoidal). The continua structure near this knot has associated the HK83-005 identification, but in our emission line maps it has only a little tail that is hardly seen. The other way around happens to knot B. Although in the emission line maps it is seen some structure, in the continuum maps only a weak contribution is present. Knot D has a clear correspondence between the continuum and the Hα emission.
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3.4. Results 71<br />
60¡DEC (arcsec)<br />
50<br />
40<br />
30<br />
20<br />
10<br />
0<br />
0 10 20 30 40 50 60 70<br />
RA (arcsec)<br />
Figure 3.16: Maps <strong>in</strong> the cont<strong>in</strong>uum near 8500 Å together with the isocontours <strong>of</strong> Hα overplotted.<br />
Map displayed <strong>in</strong> l<strong>in</strong>ear scale, while the isocontour <strong>in</strong> logarithmic scale. Contours are masked<br />
accord<strong>in</strong>gly to their emission l<strong>in</strong>e flux. The cont<strong>in</strong>uum map source comes from the (red) first po<strong>in</strong>t<strong>in</strong>g.<br />
quite similar, with the four ma<strong>in</strong> <strong>in</strong>tense knots (A, B, C and, D) well demarc<strong>at</strong>ed. The<br />
brightest knot, A, has the most extended structure, with a tail po<strong>in</strong>t<strong>in</strong>g to the north-west.<br />
This structure seems to be formed follow<strong>in</strong>g the cont<strong>in</strong>ua morphology. There are not many<br />
differences between the cont<strong>in</strong>uum maps <strong>of</strong> Hα and Hβ. The peak <strong>in</strong>tensity <strong>of</strong> the cont<strong>in</strong>uum<br />
<strong>in</strong> knot A corresponds to the same position <strong>in</strong> both emission l<strong>in</strong>e maps. From the cont<strong>in</strong>uum<br />
emission, it can be seen th<strong>at</strong> the structure <strong>of</strong> knot A def<strong>in</strong>es th<strong>at</strong> <strong>of</strong> the Hα map, with a<br />
small concentr<strong>at</strong>ion to the west <strong>of</strong> the knot, probably be<strong>in</strong>g the source <strong>of</strong> the north-west tail<br />
<strong>of</strong> this knot.<br />
Although the rest <strong>of</strong> knots have their equivalence between their emission l<strong>in</strong>e maps and<br />
cont<strong>in</strong>ua, their maximum position are not the same. A remarkable structure is the one <strong>of</strong><br />
knot C, which has an elong<strong>at</strong>ed cont<strong>in</strong>uum <strong>in</strong> a south-east to north-west direction, while the<br />
emission l<strong>in</strong>e morphology is egg-like (ellipsoidal). The cont<strong>in</strong>ua structure near this knot has<br />
associ<strong>at</strong>ed the HK83-005 identific<strong>at</strong>ion, but <strong>in</strong> our emission l<strong>in</strong>e maps it has only a little tail<br />
th<strong>at</strong> is hardly seen.<br />
The other way around happens to knot B. Although <strong>in</strong> the emission l<strong>in</strong>e maps it is seen<br />
some structure, <strong>in</strong> the cont<strong>in</strong>uum maps only a weak contribution is present. Knot D has a<br />
clear correspondence between the cont<strong>in</strong>uum and the Hα emission.