02.01.2015 Views

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 ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

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).

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!