2011
DOI: 10.1051/0004-6361/201116669
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Abundances in planetary nebulae: NGC 1535, NGC 6629, He2-108, and Tc1

Abstract: Context. Models have been made of stars of a given mass that produce planetary nebulae that usually begin on the AGB (although they may begin earlier) and run to the white dwarf stage. While these models cover the so-called dredge-up phases when nuclear reactions occur and the newly formed products are brought to the surface, it is important to compare the abundances predicted by the models with the abundances actually observed in PNe. Aims. The aim of the paper is to determine the abundances in a group of PNe… Show more

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Cited by 26 publications
(58 citation statements)
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“…By following García-Hernández et al (2012b, Eqs. (1)- (3)), we can estimate the density of C 60 molecules by assuming a spherical shell of radius (R out − R in ) and a uniform number of C 60 molecules throughout the shell. Thus, considering that L = 1480 L for Tc 1 (Pottasch et al 2011), we obtain dust temperatures (T d ) of 415 K at ∼18 au and 100 K at 301 au, where the first temperature is the C 60 excitation temperature (García-Hernández et al 2011a) and the latter temperature corresponds to the minimum temperature of the dust to be detected in the mid-IR by Spitzer. For a distance of 2 kpc, we estimate a circumstellar density of fullerenes n(C 60 ) = 0.46 cm −3 and a C 60 column density along the path (R out − R in ) of ∼2 × 10 15 cm −2 ; a lower C 60 column density of 3 × 10 14 cm −2 is obtained for L = 10 4 L .…”
Section: Electronic Transitions Of Neutral C 60mentioning
confidence: 95%
“…By following García-Hernández et al (2012b, Eqs. (1)- (3)), we can estimate the density of C 60 molecules by assuming a spherical shell of radius (R out − R in ) and a uniform number of C 60 molecules throughout the shell. Thus, considering that L = 1480 L for Tc 1 (Pottasch et al 2011), we obtain dust temperatures (T d ) of 415 K at ∼18 au and 100 K at 301 au, where the first temperature is the C 60 excitation temperature (García-Hernández et al 2011a) and the latter temperature corresponds to the minimum temperature of the dust to be detected in the mid-IR by Spitzer. For a distance of 2 kpc, we estimate a circumstellar density of fullerenes n(C 60 ) = 0.46 cm −3 and a C 60 column density along the path (R out − R in ) of ∼2 × 10 15 cm −2 ; a lower C 60 column density of 3 × 10 14 cm −2 is obtained for L = 10 4 L .…”
Section: Electronic Transitions Of Neutral C 60mentioning
confidence: 95%
“…10. Pottasch et al (2011). to the N V profile instead of P V . The statistical significance of the null field values is extensively discussed in Bagnulo et al (2012).…”
Section: Observations Data Reduction and Magnetic Field Determinationsmentioning
confidence: 99%
“…We adopted the line-ratios measured by Sharpee et al (2007) -20, Pereira & Miranda (2007) for SaSt2-3, and compiled by Pottasch et al (2011) for Tc1. The emission-line fluxes in the mid-IR wavelength range were measured by us for all objects in our sample.…”
Section: Cloudy Modeling Approachmentioning
confidence: 99%