D.J. Axon , A. Capetti , F. Macchetto , W.B. Sparks , A. Boksenberg
{"title":"The location of the hidden nucleus of NGC 1068","authors":"D.J. Axon , A. Capetti , F. Macchetto , W.B. Sparks , A. Boksenberg","doi":"10.1016/0083-6656(95)00096-8","DOIUrl":null,"url":null,"abstract":"<div><p>We present HST polarization observations of NGC 1068 obtained with the Faint Object Camera in the ultraviolet (λ ∼ 2700–3700 Å), and the Wide Field Planetary Camera in the visual (λ ∼ 5000–6000 Å), at a resolution of 0.″06 and 0.″08, respectively. The UV continuum polarization is very high, peaking at ∼ 60% in the vicinity of the emission line knot 4″.5 NE of the nucleus. To a high degree of precision the polarization vectors show the centro-symmetric pattern expected from scattering from a point source. By locating the centre of symmetry of this pattern we have determined the location of the hidden nuclear source, to an accuracy of ±0.″05, which lies 0.″65 South of the emission peak and 0.″35 South of the 12.4μ peak. A pair of highly polarized clouds (<em>P</em> ∼ 45% in the UV) lies close to the position of the scattered nuclear source and correspond to the “<em>twin cresent</em>” object seen in FOC [OIII] images. The WF/PC-I polarization images contain contributions from both the optical continuum and emission lines. Generally, the large scale polarization structure is dominated by scattered [O III] emission from knot B, except at the edge of the cavity when other NLR knots contribution. However, scattered continuum from the nucleus dominates the polarization in a narrow linear region stetching from the “<em>hidden nucleus</em>” to knot B, suggesting that there is a component to the nuclear light which is highly collimated.</p></div>","PeriodicalId":101275,"journal":{"name":"Vistas in Astronomy","volume":"40 1","pages":"Pages 29-34"},"PeriodicalIF":0.0000,"publicationDate":"1996-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0083-6656(95)00096-8","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Vistas in Astronomy","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0083665695000968","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
Abstract
We present HST polarization observations of NGC 1068 obtained with the Faint Object Camera in the ultraviolet (λ ∼ 2700–3700 Å), and the Wide Field Planetary Camera in the visual (λ ∼ 5000–6000 Å), at a resolution of 0.″06 and 0.″08, respectively. The UV continuum polarization is very high, peaking at ∼ 60% in the vicinity of the emission line knot 4″.5 NE of the nucleus. To a high degree of precision the polarization vectors show the centro-symmetric pattern expected from scattering from a point source. By locating the centre of symmetry of this pattern we have determined the location of the hidden nuclear source, to an accuracy of ±0.″05, which lies 0.″65 South of the emission peak and 0.″35 South of the 12.4μ peak. A pair of highly polarized clouds (P ∼ 45% in the UV) lies close to the position of the scattered nuclear source and correspond to the “twin cresent” object seen in FOC [OIII] images. The WF/PC-I polarization images contain contributions from both the optical continuum and emission lines. Generally, the large scale polarization structure is dominated by scattered [O III] emission from knot B, except at the edge of the cavity when other NLR knots contribution. However, scattered continuum from the nucleus dominates the polarization in a narrow linear region stetching from the “hidden nucleus” to knot B, suggesting that there is a component to the nuclear light which is highly collimated.