2002MNRAS.337..499Z


Query : 2002MNRAS.337..499Z

2002MNRAS.337..499Z - Mon. Not. R. Astron. Soc., 337, 499-518 (2002/December-1)

A spectroscopic study of the bipolar planetary nebula Mz 3.

ZHANG Y. and LIU X.-W.

Abstract (from CDS):

We have obtained a medium-resolution, deep optical long-slit spectrum of the bipolar planetary nebula Mz 3. The spectrum covers the wavelength range 3420-7400Å. Over 200 emission lines have been detected, many of them permitted and forbidden transitions from Fe+, Fe 2+ and Fe3+ and other iron-group elements. The spectra have been used to determine nebular thermal and density structures and elemental abundances.

The very rich and prominent [Feiii] emission lines observed in the optical spectrum of Mz 3 are found to originate exclusively from an unresolved emission region centred on the central star. The relative intensities of [Feiii] lines arising from the same upper level are in good agreement with the theoretical predictions. The [Feiii] lines detected in Mz 3, arising from levels of different excitation energies and critical densities, provide powerful diagnostic tools to probe the physical conditions in the central emitting region. We find that all the observed [Feiii] diagnostic line ratios consistently yield an electron temperature of Te= 11 000 K and a density of logNe(cm –3) = 6.5 . The latter value is close to the densities where the ratios of these [Feiii] diagnostic lines are most sensitive to density variations, suggesting that the density in the central emission core could be even higher. In contrast, all the other standard nebular density- and temperature-diagnostic line ratios, all of lower critical densities than the [Feiii] lines and therefore only useful at densities ≤106 cm –3, yield consistently lower electron densities, with the resultant values correlating with their critical densities. This indicates that the central dense emission core has a highly stratified density structure such that forbidden lines of relatively low critical densities are collisionally suppressed in high-density regions. Given the highly stratified thermal and density structures of the core emission region, no reliable elemental abundances can be determined for this region, except possibly for iron, for which we find an abundance of approximately half the solar value.

In contrast to the dense central core, emission from the extended bipolar lobes of Mz 3 are well represented by a mean electron temperature of 6800 K and density of 5200 cm–3. The elemental abundances derived for this region, on a logarithmic scale where H = 12, are He = 10.93, C = 8.41, N = 8.37, O = 8.50, Ne = 7.64, S = 7.15, Cl = 5.28 and Ar = 7.14. In all cases, the abundances are close to the average values deduced for Galactic planetary nebulae. In particular, there is no evidence of He enrichment, as claimed in previous studies. The newly derived heavy-element abundances are significantly higher than those published in the literature. In those earlier studies, as a result of the contamination of emission from the dense central core, the average electron temperature in Mz 3 was significantly overestimated, resulting in grossly underestimated heavy-element abundances. However, Mz 3 does seem to have a relatively high N/O abundance ratio, in line with the result derived from the ISO observations of the far-infrared fine-structure lines.


Abstract Copyright: RAS

Journal keyword(s): line: identification - ISM: abundances - ISM: lines and bands - planetary nebulae: individual: Mz 3

Simbad objects: 20

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Number of rows : 20
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 RAFGL 618 pA* 04 42 53.6242032600 +36 06 53.400902220   16.32   12.59   C-rich 1027 0
2 * tet01 Ori C SB* 05 35 16.4662967280 -05 23 22.921811880 4.20 5.15 5.13 4.91 4.73 O7Vp 1479 1
3 WRAY 16-40 PN 09 18 01.3172902776 -54 39 29.165596128   14 15.00     ~ 81 0
4 V* RW LMi C* 10 16 02.2777043904 +30 34 19.045098516       15.27   C4,3e 411 0
5 PN Th 2-B PN 13 28 38.8514280930 -63 49 46.321978384       15.72 14.54 ~ 39 0
6 WRAY 16-147 Sy* 14 11 52.0604355768 -51 26 24.187122024     14.20     ~ 240 1
7 PN Mz 3 PN 16 17 13.3915382496 -51 59 10.711893480   10.8 14.00     O9.5 359 0
8 PN M 2-9 PN 17 05 37.96152 -10 08 32.5068           ~ 532 0
9 NGC 6302 PN 17 13 44.5 -37 06 11           O-rich 821 2
10 NGC 6543 PN 17 58 33.4039587288 +66 37 58.750734000   11.09 11.28     [WC] 1197 2
11 NGC 6537 PN 18 05 13.104 -19 50 34.88     13.58     ~ 438 1
12 PN Cn 3-1 PN 18 17 34.1015035728 +10 09 03.304908396   12.93 12.49 12.35   07Ib(f) 224 0
13 PN Hu 2-1 PN 18 49 47.5610183328 +20 50 39.396894756   12.369 11.126 12.30   ~ 286 0
14 PN M 4-12 PN 19 13 05.4493583551 +15 46 39.915114808   16.327 15.095 15.678   ~ 100 0
15 Hen 2-437 PN 19 32 57.6040534728 +26 52 43.087922580           ~ 98 1
16 Min 1-92 pA* 19 36 18.9295687968 +29 32 49.785288144 12.13 12.35 11.75 11.54   B0.5IV[e] 267 0
17 IC 4997 PN 20 20 08.7557973960 +16 43 53.698933380   11.94 11.15     [WC7/8] 555 0
18 NGC 7027 PN 21 07 01.571952 +42 14 10.47120   10.358 8.831 10.157   ~ 2541 1
19 V* V645 Cyg Ae* 21 39 58.2745507632 +50 14 21.042184668   14.23 13.10 13.82   O6/9eq 279 0
20 NGC 7293 PN 22 29 38.5454047152 -20 50 13.747242408 11.894 13.158 13.524 13.689 13.898 DAO.5 983 1

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