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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92 3 • IFS <strong>of</strong> a GEHR <strong>in</strong> NGC 6946<br />
6584 Å l<strong>in</strong>es assum<strong>in</strong>g th<strong>at</strong> T([Nii]) ≈ T([Oii]). Then, the total N abundance was derived<br />
under the follow<strong>in</strong>g assumption:<br />
N<br />
O ≈ N +<br />
O +<br />
Neon is only visible <strong>in</strong> the spectra via the [Neiii] emission l<strong>in</strong>e <strong>at</strong> λ3869 Å. For this ion,<br />
we took the electron temper<strong>at</strong>ure <strong>of</strong> [Oiii], as represent<strong>at</strong>ive <strong>of</strong> the high excit<strong>at</strong>ion zone. The<br />
total abundance <strong>of</strong> neon was calcul<strong>at</strong>ed us<strong>in</strong>g the follow<strong>in</strong>g expression for the ICF (Pérez-<br />
Montero et al., 2007):<br />
ICF (Ne 2+ ) ≈ 0.753 + 0.142 ·<br />
O 2+<br />
O + + O 2+ + 0.171 · O+ + O 2+<br />
O 2+<br />
This formula considers the overestim<strong>at</strong>e <strong>of</strong> Ne/H <strong>in</strong> objects with low excit<strong>at</strong>ion, where<br />
the charge transfer between O 2+ and H 0 becomes important (Izotov et al., 2004).<br />
The only accessible emission l<strong>in</strong>es <strong>of</strong> argon <strong>in</strong> the optical spectra <strong>of</strong> <strong>ionized</strong> <strong>regions</strong> correspond<br />
to Ar 2+ and Ar 3+ . However, <strong>in</strong> the <strong>in</strong>tegr<strong>at</strong>ed spectra <strong>of</strong> the knots only [Ariii] λ 7136 Å<br />
was measured and the abundance <strong>of</strong> Ar 2+ was calcul<strong>at</strong>ed assum<strong>in</strong>g th<strong>at</strong> T([Ariii]) ≈ T([Siii])<br />
(Garnett, 1992). As already described <strong>in</strong> section 3.4.7, [Ariv] λ 4741 Å was present <strong>in</strong> some<br />
knots and subtracted to their WR blue bump flux, but their contribution was small to yield<br />
any accur<strong>at</strong>e abundance determ<strong>in</strong><strong>at</strong>ion. The total abundance <strong>of</strong> Ar was then calcul<strong>at</strong>ed us<strong>in</strong>g<br />
the ICF(Ar 2+ ) derived from photo-ioniz<strong>at</strong>ion models by Pérez-Montero et al. (2007):<br />
(<br />
ICF (Ar 2+ ) = 0.749 + 0.507 · 1 −<br />
O 2+ )<br />
(<br />
O + + O 2+ + +0.0604 · 1 −<br />
O 2+<br />
O + + O 2+ ) −1<br />
F<strong>in</strong>ally, for iron the [Feiii] λ 4658 Å emission l<strong>in</strong>e was used and the electron temper<strong>at</strong>ure<br />
<strong>of</strong> [Oiii]. We have taken the ICF(Fe 2+ ) from Rodríguez and Rub<strong>in</strong> (2004), which yields<br />
ICF (F e 2+ ) =<br />
( ) O<br />
+ 0.09 ( )<br />
O 2+ 1 + O2+<br />
O +<br />
The ionic and total abundances for each observed element for knots A, B, and, C are<br />
given <strong>in</strong> Table 3.9, along with their correspond<strong>in</strong>g errors.<br />
3.5 Discussion<br />
3.5.1 Mass <strong>of</strong> the <strong>ionized</strong> gas<br />
We have calcul<strong>at</strong>ed the Hα lum<strong>in</strong>osities for the four knots from our observed values,<br />
correct<strong>in</strong>g for ext<strong>in</strong>ction accord<strong>in</strong>g to the values found from the spectroscopic analysis. The