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

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20 2 • The star form<strong>at</strong>ion history <strong>of</strong> NGC 5471<br />

Figure 2.5: Plot <strong>of</strong> the eleven polygons, limit<strong>in</strong>g the <strong>different</strong> areas where the <strong>in</strong>tegr<strong>at</strong>ed magnitudes<br />

are computed. The numbers belong to our own def<strong>in</strong>ition while the A, B, C, D and E letters are the<br />

knots identified by Skillman (1985). The hypernova is loc<strong>at</strong>ed <strong>in</strong> knot 6.<br />

cm −2 s −1 Å −1 (14.24 ± 0.05 AB magnitudes).<br />

In order to use these values <strong>in</strong> the analysis, we need to transform AB magnitudes to the<br />

VEGAMAG system. The transform<strong>at</strong>ion formula is (Maíz-Apellániz, 2007):<br />

AB p = (m p − ZP p ) + AB p (V ega) (2.1)<br />

where AB p is the magnitude <strong>of</strong> the object <strong>in</strong> the AB system and filter passband p, m p the<br />

magnitude <strong>of</strong> the object <strong>in</strong> filter p us<strong>in</strong>g Vega as reference spectral energy distribution (SED),<br />

ZP p is the zero po<strong>in</strong>t <strong>of</strong> the p filter <strong>in</strong> the Vega system and AB p (Vega) is the AB magnitude<br />

<strong>of</strong> Vega <strong>in</strong> filter p. This magnitude is given by:

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