ngc1068的隐核位置

D.J. Axon , A. Capetti , F. Macchetto , W.B. Sparks , A. Boksenberg
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引用次数: 2

摘要

我们介绍了NGC 1068的HST偏振观测结果,这些观测结果是用微弱天体相机在紫外波段(λ ~ 2700-3700 Å)和宽视场行星相机在可见光波段(λ ~ 5000-6000 Å)获得的,分辨率为0。″06和0。“08年,分别。紫外连续极化非常高,在发射线结4″.5附近达到约60%的峰值原子核的NE。在较高的精度下,偏振矢量显示了点源散射所期望的中心对称模式。通过定位这个图案的对称中心,我们已经确定了隐藏核源的位置,精度为±0。″05,等于0。″65排放峰以南和0。″35 12.4μ峰以南。一对高度极化的云(紫外线P ~ 45%)靠近散射核源的位置,对应于FOC [OIII]图像中看到的“双新月”物体。WF/ pc - 1偏振图像包含了光连续线和发射线的贡献。一般来说,大尺度极化结构主要由B结的散射[O III]发射主导,除了在腔的边缘有其他NLR节的贡献。然而,在从“隐藏核”延伸到结B的狭窄线性区域中,来自原子核的散射连续体主导了偏振,这表明原子核光存在高度准直的成分。
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The location of the hidden nucleus of NGC 1068

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.

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