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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>

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