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

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128 4 • Long-slit spectrophotometry <strong>of</strong> multiple knots <strong>of</strong> Hii <strong>galaxies</strong><br />

J1657 Knot A J1657 Knot B J1657 Knot C<br />

He + /H + (λ4471) 0.093±0.007 0.085±0.009 0.094±0.009<br />

He + /H + (λ5876) 0.085±0.003 0.079±0.002 0.093±0.003<br />

He + /H + (λ6678) 0.086±0.005 0.077±0.003 0.084±0.005<br />

He + /H + (λ7065) 0.093±0.005 0.086±0.006 0.105±0.010<br />

He + /H + (Adopted) 0.087±0.005 0.080±0.005 0.092±0.009<br />

He 2+ /H + (λ4686) 0.0011±0.0001 0.0028±0.0006 0.0015±0.0002<br />

(He/H) 0.088±0.008 0.080±0.008 0.092±0.009<br />

Table 4.6: Ionic and total chemical abundances for helium for the knots <strong>of</strong> J1657.<br />

Ionic and total chemical abundances from forbidden l<strong>in</strong>es<br />

The oxygen ionic abundance r<strong>at</strong>ios, O + /H + and O 2+ /H + , have been derived from the<br />

[Oii] λλ 3727,29 Å and [Oiii] λλ 4959, 5007 Å l<strong>in</strong>es respectively us<strong>in</strong>g for each ion its correspond<strong>in</strong>g<br />

temper<strong>at</strong>ure 3 .<br />

At the temper<strong>at</strong>ures derived for our observed <strong>galaxies</strong>, most <strong>of</strong> the oxygen is <strong>in</strong> the form<br />

<strong>of</strong> O + and O 2+ , therefore the approxim<strong>at</strong>ion:<br />

has been used.<br />

O<br />

H = O+ + O 2+<br />

H +<br />

In the same way, we have derived S + /H + and S 2+ /H + , abundances us<strong>in</strong>g t([Sii]) and<br />

t([Siii]) values and the fluxes <strong>of</strong> the [Sii] emission l<strong>in</strong>es <strong>at</strong> λλ 6717,6731 Å and the near-IR<br />

[Siii] λλ 9069, 9532 Å l<strong>in</strong>es respectively. For IIZw71, we have assumed th<strong>at</strong> T([Sii]) ≈ T([Oii]).<br />

Unlike oxygen, for sulphur a rel<strong>at</strong>ively important contribution from S 3+ may be expected<br />

depend<strong>in</strong>g on the nebular excit<strong>at</strong>ion. The total sulphur abundance has been calcul<strong>at</strong>ed us<strong>in</strong>g<br />

an ICF for S + +S 2+ accord<strong>in</strong>g to the formula by Barker (1980), which is based on the photoioniz<strong>at</strong>ion<br />

models by Stasińska (1978):<br />

ICF (S + + S 2+ ) =<br />

[ (<br />

O 2+ ) α ] −1/α<br />

1 − 1 −<br />

O + + O 2+<br />

where α = 2.5 gives the best fit to the scarce observ<strong>at</strong>ional d<strong>at</strong>a on S 3+ abundances (Pérez-<br />

Montero et al., 2006). Tak<strong>in</strong>g this ICF as a function <strong>of</strong> the r<strong>at</strong>io O 2+ /O <strong>in</strong>stead <strong>of</strong> O + /O<br />

reduces the propag<strong>at</strong>ed error for this quantity.<br />

The ionic abundance <strong>of</strong> nitrogen, N + /H + has been derived from the <strong>in</strong>tensities <strong>of</strong> the<br />

λλ 6548,6584 Å l<strong>in</strong>es and along with the assumption T e ([Nii]) ≈ T e ([Oii]).<br />

The N/O abundance r<strong>at</strong>io has been derived under the assumption th<strong>at</strong><br />

3 As <strong>in</strong> Chapter 3, we have used fitt<strong>in</strong>gs to the ionic task results. Aga<strong>in</strong>, see Appendix B for details.

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