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Spatially Resolved Far-ultraviolet Spectroscopy Of The Nuclear Region Of Ngc 1068

机译:Ngc 1068核区的空间分辨远紫外光谱

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We carry out high-resolution FUSE spectroscopy of the nuclear region of NGC 1068. The first set of spectra was obtained with a 30" square aperture that collected all emission from the narrow-line region. The data reveal a strong broad O VI component of FWHM ~3500 km s~(-1) and two narrow O VI λλ1031,1037 components of ~350 km s~(-1). The C III λ911 and N III λ991 emission lines in this spectrum can be fitted with a narrow component of FWHM ~ 1000 km s~(-1) and a broad one of ~2500 km s~(-1). Another set of seven spatially resolved spectra was made using a long slit of 1.25" × 20" at steps of ~1" along the axis of the emission-line cone. We find the following: (1) Major emission lines in the FUSE wavelength range consist of a broad and a narrow component. (2) There is a gradient in the velocity field for the narrow O VI component of ~200 km s~(-1) from ~2" southwest of the nucleus to ~4" northeast. A similar pattern is also observed with the broad O VI component, with a gradient of ~3000 km s~(-1). These are consistent with the HST STIS findings and suggest a biconical structure in which the velocity field is mainly radial outflow. (3) A major portion of the C III and N III line flux is produced in the compact core. They are therefore not effective temperature diagnostics for the conical region. (4) The best-fit UV continuum suggests virtually no reddening, and the He II I(λ 1640)/I(λ 1085) ratio suggests a consistently low extinction factor across the cone. At ~2" northeast of the nucleus there is a region characterized by (a) a strong Lyα flux but normal C IV flux, (b) a broad O VI line, and (c) a significantly enhanced C III flux.
机译:我们对NGC 1068的核区域进行了高分辨率FUSE光谱分析。第一组光谱是使用30英寸见方的孔径获得的,该孔径收集了窄线区域的所有发射。数据显示了强烈的宽OVI成分FWHM〜3500 km s〜(-1)和两个狭窄的O VIλλ1031,1037分量〜350 km s〜(-1)。该光谱中的C IIIλ911和N IIIλ991发射线可以适合一个窄分量FWHM〜1000 km s〜(-1)的宽幅和〜2500 km s〜(-1)的宽幅宽的另一幅。使用1.25“×20”的长缝以〜1的步长绘制了另一组七个空间分辨的光谱沿着发射线锥的轴。我们发现以下情况:(1)FUSE波长范围内的主要发射线由宽和窄组成。 (2)从原子核西南2〜东北4〜200 km s〜(-1)的狭窄O VI分量在速度场中存在一个梯度。在较宽的O VI分量上也观察到了类似的模式,其梯度为〜3000 km s〜(-1)。这些与HST STIS的发现是一致的,并提出了一种双锥形结构,其中速度场主要是径向流出。 (3)C III和N III线通量的主要部分在紧凑型磁芯中产生。因此,它们对于锥形区域不是有效的温度诊断。 (4)最合适的UV连续体表明几乎没有变红,而He II I(λ1640)/ I(λ1085)的比值表明整个圆锥上的消光因子始终较低。在原子核东北约2“处有一个区域,其特征是(a)强的Lyα通量但C IV通量正常,(b)宽的O VI线,以及(c)C III通量显着增强。

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