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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136 4 • Long-slit spectrophotometry <strong>of</strong> multiple knots <strong>of</strong> Hii <strong>galaxies</strong><br />
(2005) were derived us<strong>in</strong>g empirical calibr<strong>at</strong>ions s<strong>in</strong>ce no temper<strong>at</strong>ure sensitive l<strong>in</strong>es were<br />
observed.<br />
The logarithmic N/O r<strong>at</strong>ios found for J1657 are -1.23 ± 0.11, -1.35 ± 0.16 and -1.36 ±<br />
0.15 for knots A, B, and C, respectively, which are remarkably constant. The derived values<br />
are on the high log(N/O) side <strong>of</strong> the distribution for this k<strong>in</strong>d <strong>of</strong> objects (see Figure 4.15).<br />
For IIZw71, although the difference between knots B and C is <strong>of</strong> 0.2 dex, due to the large<br />
errors, it can be consider as well fairly constant.<br />
In general, the common procedure <strong>of</strong> obta<strong>in</strong><strong>in</strong>g t e ([Oii]) from t e ([Oiii]) us<strong>in</strong>g Stasińska<br />
(1990) rel<strong>at</strong>ion and assum<strong>in</strong>g t e ([Oii]) = t e ([Nii]), yields N/O r<strong>at</strong>ios larger than us<strong>in</strong>g the<br />
measured t e ([Oii]) values s<strong>in</strong>ce, <strong>in</strong> most cases, the model sequence over-predicts t e ([Oii]). In<br />
our particular case, as we have seen, for the three knots <strong>of</strong> J1657 t e ([Oii]) is under-predicted<br />
by Stasińska (1990) models; for Knot B the difference is more than 2000 K. This would<br />
decrease the N/O r<strong>at</strong>io by more than 0.1 dex.<br />
The log(S/O) r<strong>at</strong>ios found are the quite similar for Knots A and B <strong>of</strong> J1657, with -1.53<br />
and -1.57, respectively, and higher for Knot C, with -1.32. The average error is 0.12. For<br />
IIZw71, both knots shows a very similar value. They are consistent with log(S/O) ⊙ = -1.36,<br />
the solar value (Grevesse and Sauval, 1998) with<strong>in</strong> the observ<strong>at</strong>ional errors (see Figure 4.15).<br />
The logarithmic Ne/O r<strong>at</strong>io is remarkably constant <strong>of</strong> both objects, with a mean value<br />
<strong>of</strong> 0.75, despite, for example, the differences <strong>in</strong> oxygen abundances between knot A and the<br />
other two <strong>in</strong> J1657. They are consistent with solar value, log(Ne/O) = -0.61 dex 4 , as shown<br />
<strong>in</strong> Figure 4.16.<br />
F<strong>in</strong>ally, the Ar/O r<strong>at</strong>ios found show a very similar value for Knot A and B, while Knot<br />
C has a r<strong>at</strong>io higher by 0.2 dex. Both knots <strong>of</strong> IIZw71 have the same r<strong>at</strong>io. The mean value<br />
is consistent with solar 5 (see Figure 4.16).<br />
4.4.2 Chemical abundances from empirical calibr<strong>at</strong>ors for Knots A and<br />
D <strong>of</strong> IIZw71<br />
The emission-l<strong>in</strong>e spectra <strong>of</strong> the four star-form<strong>in</strong>g knots <strong>in</strong> IIZw71 are remarkably similar,<br />
imply<strong>in</strong>g similar values for ioniz<strong>at</strong>ion parameter, ioniz<strong>at</strong>ion temper<strong>at</strong>ure, and chemical<br />
abundances. We derived the ioniz<strong>at</strong>ion parameters from the r<strong>at</strong>io <strong>of</strong> the [Oii] and [Oiii] l<strong>in</strong>es<br />
accord<strong>in</strong>g to the expression given <strong>in</strong> Díaz et al. (2000) (see Chapter §3). They are similar<br />
<strong>in</strong> all the knots rang<strong>in</strong>g from 6.42×10 −4 for knot A to 9.67×10 −4 for knot C. Us<strong>in</strong>g these<br />
values, the corrected Hα fluxes, and the sizes <strong>of</strong> the <strong>regions</strong> from Hα images we can calcul<strong>at</strong>e<br />
the density <strong>of</strong> the emitt<strong>in</strong>g gas (Diaz et al., 1991). This is similar for the four knots with a<br />
value <strong>of</strong> about 20 particles · cm −3 , consistent with the upper limits we derived from the r<strong>at</strong>io<br />
<strong>of</strong> the [Sii] l<strong>in</strong>es and provid<strong>in</strong>g fill<strong>in</strong>g factor for the gas <strong>of</strong> a few times 10 −2 , values common<br />
4 Oxygen from Allende Prieto et al. (2001) and neon from Grevesse and Sauval (1998).<br />
5 Oxygen from Allende Prieto et al. (2001) and argon from Grevesse and Sauval (1998).