2005MNRAS.362..424W


Query : 2005MNRAS.362..424W

2005MNRAS.362..424W - Mon. Not. R. Astron. Soc., 362, 424-454 (2005/September-2)

The abundance discrepancy - recombination line versus forbidden line abundances for a northern sample of galactic planetary nebulae.

WESSON R., LIU X.-W. and BARLOW M.J.

Abstract (from CDS):

We present deep optical spectra of 23 galactic planetary nebulae, which are analysed in conjunction with archival infrared and ultraviolet spectra. We derive nebular electron temperatures based on standard collisionally excited line (CEL) diagnostics as well as the hydrogen Balmer jump and find that, as expected, the Balmer jump almost always yields a lower temperature than the [Oiii] nebular-to-auroral line ratio. We also make use of the weak temperature dependence of helium and Oii recombination line ratios to further investigate the temperature structure of the sample nebulae. We find that, in almost every case, the derived temperatures follow the relation, which is the relation predicted by two-component nebular models in which one component is cold and hydrogen-deficient. Te(Oii) may be as low as a few hundred Kelvin, in line with the low temperatures found for the hydrogen-deficient knots of Abell 30 by Wesson, Liu and Barlow.

Elemental abundances are derived for the sample nebulae from both CELs and optical recombination lines (ORLs). ORL abundances are higher than CEL abundances in every case, by factors ranging from 1.5 to 12. Five objects with O2+ abundance discrepancy factors greater than 5 are found. DdDm 1 and Vy 2-2 are both found to have a very large abundance discrepancy factor of 11.8.

We consider the possible explanations for the observed discrepancies. From the observed differences between Te(Oiii) and Te(BJ), we find that temperature fluctuations cannot resolve the abundance discrepancies in 22 of the 23 sample nebulae, implying some additional mechanism for enhancing ORL emission. In the one ambiguous case, the good agreement between abundances derived from temperature-insensitive infrared lines and temperature-sensitive optical lines also points away from temperature fluctuations being present. The observed recombination line temperatures, the large abundance discrepancies and the generally good agreement between infrared and optical CEL abundances all suggest instead the existence of a cold hydrogen-deficient component within the `normal' nebular gas. The origin of this component is as yet unknown.


Abstract Copyright: 2005 RAS

Journal keyword(s): ISM: abundances - planetary nebulae: general

Simbad objects: 36

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Number of rows : 36
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 PN Hu 1-1 PN 00 28 15.435 +55 57 54.48           ~ 169 1
2 IC 1747 PN 01 57 35.6899203048 +63 19 18.447328776   15.8 15.4     [WC4] 269 2
3 IC 351 PN 03 47 32.9806443144 +35 02 48.639127308   13.11 12.27 14.35   Of(H) 264 0
4 IC 2003 PN 03 56 21.9884187048 +33 52 30.759977028   13.11 11.87 13.44   [WC3?] 261 0
5 NGC 1501 PN 04 06 59.3920909320 +60 55 14.278542024   15.17 13.0     [WO4] 314 1
6 PN A66 30 PN 08 46 53.4639874872 +17 52 46.369394580   14.23 14.30 13.47   [WC5] 431 0
7 HZ 44 HS* 13 23 35.2629445608 +36 07 59.544140304 10.186 11.42 11.65 12.00 11.995 sdBN0VIIHe28 439 0
8 PN Mz 3 PN 16 17 13.3915382496 -51 59 10.711893480   10.8 14.00     O9.5 359 0
9 NGC 6153 PN 16 31 30.5708444544 -40 15 12.646208700   10.7 15.55     ~ 320 0
10 PN DdDm 1 PN 16 40 18.1517248296 +38 42 20.033859348   14.0 13.90     sd+G/K 153 0
11 PN Vy 1-2 PN 17 54 22.98 +27 59 58.1           ~ 118 0
12 NGC 6543 PN 17 58 33.4039587288 +66 37 58.750734000   11.09 11.28     [WC] 1197 2
13 PN M 2-24 PN 18 02 02.8945854456 -34 27 47.275175592   15.62 14.60 15.29   ~ 100 0
14 PN M 1-42 PN 18 11 04.99 -28 58 59.1   13.1 14.00     ~ 221 0
15 PN Cn 3-1 PN 18 17 34.1015035728 +10 09 03.304908396   12.93 12.49 12.35   07Ib(f) 224 0
16 PN M 2-36 PN 18 17 41.43 -29 08 19.9         17.012 ~ 140 0
17 PN M 3-27 PN 18 27 48.2638650624 +14 29 06.066648996           ~ 84 0
18 PN Hf 2-2 PN 18 32 30.9015918072 -28 43 20.276106312     15.90     ~ 110 0
19 PN Hu 2-1 PN 18 49 47.5610183328 +20 50 39.396894756   12.369 11.126 12.30   ~ 286 0
20 PN Sp 4-1 PN 19 00 26.5460404944 +38 21 07.280102016       15.26   O? 40 0
21 IC 4846 PN 19 16 28.2266496960 -09 02 36.677150592           ~ 221 0
22 PN Vy 2-2 PN 19 24 22.2390166933 +09 53 56.259102426   14.02 12.65 13.38   O-rich 274 0
23 PN M 3-34 PN 19 27 01.8981450048 -06 35 04.739628516           ~ 70 1
24 NGC 6803 PN 19 31 16.4826019750 +10 03 21.620200381   13.034 11.616 13.242   ~ 254 0
25 NGC 6807 PN 19 34 33.53 +05 41 02.5     12     ~ 144 0
26 PN M 1-73 PN 19 41 09.2937490896 +14 56 58.980006096           O3.5If 85 1
27 PN M 1-74 PN 19 42 18.78 +15 09 08.3   12.8       ~ 127 0
28 NGC 6833 PN 19 49 46.5667474512 +48 57 40.113276876           ~ 181 0
29 NGC 6879 PN 20 10 26.6930056361 +16 55 21.272110541   13.661 12.540 14.075   O3f(He) 157 0
30 NGC 6891 PN 20 15 08.8435405584 +12 42 15.584146740   12.11 12.51     O3Ib(f*) 405 0
31 NGC 7009 PN 21 04 10.8155187648 -11 21 48.580157556   12.48 12.07     ~ 1020 1
32 NGC 7026 PN 21 06 18.5723414928 +47 51 06.774735780   15.33 15.1     [WC3] 427 1
33 BD+28 4211 HS* 21 51 11.0221915656 +28 51 50.367627468 8.922 10.25 10.58 10.656 10.831 sdO2VIIIHe5 837 0
34 IC 5217 PN 22 23 55.7180137224 +50 58 00.464340252     15.5     [WC7] 314 0
35 PN Me 2-2 PN 22 31 43.6753782000 +47 48 03.836846628   9.3       ~ 160 0
36 Feige 110 HS* 23 19 58.3996844256 -05 09 56.171142864 10.360 11.45 11.50 11.970 12.145 sdO8VIIIHe5 673 1

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