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dc.contributor.authorJi, Xihanpt_BR
dc.contributor.authorYan, Renbinpt_BR
dc.contributor.authorBundy, Kevinpt_BR
dc.contributor.authorBoquien, Médéricpt_BR
dc.contributor.authorSchaefer, Adam L.pt_BR
dc.contributor.authorBelfiore, Francescopt_BR
dc.contributor.authorBershady, Matthew A.pt_BR
dc.contributor.authorDrory, Nivpt_BR
dc.contributor.authorLi, Chengpt_BR
dc.contributor.authorWestfall, Kyle B.pt_BR
dc.contributor.authorLin, Zesenpt_BR
dc.contributor.authorBizyaev, D.pt_BR
dc.contributor.authorLaw, David R.pt_BR
dc.contributor.authorRiffel, Rogériopt_BR
dc.contributor.authorRiffel, Rogemar Andrépt_BR
dc.date.accessioned2023-07-29T03:35:45Zpt_BR
dc.date.issued2023pt_BR
dc.identifier.issn0004-6361pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/262831pt_BR
dc.description.abstractA fundamental assumption adopted in nearly every extragalactic study that analyzes optical emission lines is that the attenuation of different emission lines can be described by a single attenuation curve, scaled by a single reddening parameter, usually E(B − V). Here we show this assumption fails in many cases with important implications for derived results. We developed a new method to measure the differential nebular attenuation among three kinds of transitions: the Balmer lines of hydrogen; high-ionization transitions (>13.6 eV) including [Ne iii], [O iii], and [S iii]; and low-ionization transitions (.13.6 eV) including [O ii], [N ii], and [S ii]. This method bins the observed data in a multidimensional space spanned by attenuation-insensitive line ratios. Within each small bin, the variations in nebular parameters such as the metallicity and ionization parameter are negligible compared to the variation in the nebular attenuation. This allowed us to measure the nebular attenuation using both forbidden lines and Balmer lines. We applied this method to a sample of 2.4 million star-forming (SF) spaxels from the Mapping Nearby Galaxies at Apache Point Observatory (MaNGA) survey. We found that the attenuation of high ionization lines and Balmer lines can be well described by a single Fitzpatrick (1999, PASP, 111, 63) extinction curve with RV = 3.1. However, no single attenuation curve can simultaneously account for these transitions and the derived attenuation of low-ionization lines. This strongly suggests that different lines have different effective attenuations, likely because spectroscopy at hundreds of parsecs to kiloparsecs of resolution mixes multiple physical regions that exhibit different intrinsic line ratios and different levels of attenuation. As a result, the assumption that different lines follow the same attenuation curve breaks down. Using a single attenuation curve determined by Balmer lines to correct attenuation-sensitive forbidden line ratios could bias the nebular parameters derived by 0.06–0.25 dex at AV = 1, depending on the details of the dust attenuation model. Observations of a statistically large sample of H ii regions with high spatial resolutions and large spectral coverage are vital for improved modeling and deriving accurate corrections for this effect.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofAstronomy and astrophysics. Les Ulis. Vol. 670 (Feb. 2023), A125, 28 p.pt_BR
dc.rightsOpen Accessen
dc.subjectPoeira cosmicapt_BR
dc.subjectDusten
dc.subjectExtinção interestelarpt_BR
dc.subjectExtinctionen
dc.subjectH II regionsen
dc.subjectMeio interestelarpt_BR
dc.subjectISM: lines and bandsen
dc.titleThe need for multicomponent dust attenuation in modeling nebular emission : constraints from SDSS-IV MaNGApt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb001171264pt_BR
dc.type.originEstrangeiropt_BR


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