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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3.3. D<strong>at</strong>a Reduction 55<br />
2<br />
1<br />
7<br />
37<br />
19<br />
Flux calibr<strong>at</strong>ion r<strong>at</strong>ios<br />
1<br />
BD+28◦ 4241<br />
airmass = 1.37<br />
A V = 0.24<br />
One po<strong>in</strong>t<strong>in</strong>g<br />
Mosaic<br />
7<br />
19<br />
5000 5500 6000 6500 7000<br />
Wavelength (◦A)<br />
37<br />
Figure 3.9: Flux r<strong>at</strong>ios <strong>of</strong> the standard star BD+28 ◦ 4211 for the flux calibr<strong>at</strong>ion <strong>in</strong> the blue range.<br />
For the sake <strong>of</strong> clarity, only a fraction <strong>of</strong> the full wavelength coverage is shown. Solid (blue) l<strong>in</strong>es<br />
represent flux r<strong>at</strong>ios for the extraction <strong>of</strong> flux around the most <strong>in</strong>tense fiber for 1, 7, 19 and 37 fibers<br />
<strong>in</strong> the case <strong>of</strong> a one-po<strong>in</strong>t<strong>in</strong>g frame. Dashed (green) l<strong>in</strong>es represents flux r<strong>at</strong>ios for the same number<br />
<strong>of</strong> extracted fibers <strong>in</strong> the case <strong>of</strong> a mosaic <strong>of</strong> three exposures. Numbers <strong>in</strong> each curve <strong>in</strong>dic<strong>at</strong>e the<br />
number <strong>of</strong> fibers used <strong>in</strong> the extraction for each curve. The flux r<strong>at</strong>io for the one-fiber extraction is<br />
the same <strong>in</strong> both cases s<strong>in</strong>ce it corresponds to the same fiber.<br />
the one-po<strong>in</strong>t<strong>in</strong>g frame <strong>of</strong> the standard star has space <strong>in</strong> between the fibers not covered by<br />
them. Although several fibers can be extracted, a significant flux could be lost. In the lower<br />
figures, selection <strong>of</strong> 37 fibers along concentric r<strong>in</strong>gs around the most <strong>in</strong>tense fiber <strong>in</strong> a mosaic<br />
<strong>of</strong> three exposures shows how the placement <strong>of</strong> the fibers covers all the FOV. Add<strong>in</strong>g all<br />
these fibers should recover most <strong>of</strong> the flux from the star.<br />
The effect <strong>of</strong> flux losses when the IFU does not cover the entire FOV can be see <strong>in</strong><br />
Figure 3.9. Solid (blue) l<strong>in</strong>es represents flux r<strong>at</strong>ios obta<strong>in</strong>ed from the extraction <strong>of</strong> flux<br />
around the most <strong>in</strong>tense fiber for 1, 7, 19 and 37 fibers <strong>in</strong> the case <strong>of</strong> a one-po<strong>in</strong>t<strong>in</strong>g frame.<br />
The extraction is done <strong>in</strong> <strong>in</strong>creas<strong>in</strong>g concentric r<strong>in</strong>gs around the most <strong>in</strong>tense fiber, as shown<br />
<strong>in</strong> Figure 3.8. Dashed (green) l<strong>in</strong>es stand for the flux r<strong>at</strong>ios for the same number <strong>of</strong> extracted<br />
fibers <strong>in</strong> the case <strong>of</strong> a mosaic <strong>of</strong> three exposures. The flux r<strong>at</strong>io curve for the one-fiber<br />
extraction curve is the same s<strong>in</strong>ce corresponds to the same fiber. As is clearly seen, there<br />
is a big gap between the flux r<strong>at</strong>ios for a one-po<strong>in</strong>t<strong>in</strong>g frame and a mosaic one. The mean<br />
difference is by more than a factor <strong>of</strong> 2.5. This confirms the flux losses and reliability <strong>of</strong>