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首页> 外文期刊>The Astrophysical journal >HUBBLE SPACE TELESCOPE FAINT OBJECT SPECTROGRAPH OPTICAL AND ULTRAVIOLET SPECTROSCOPY OF THE BOW SHOCK HH 47A
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HUBBLE SPACE TELESCOPE FAINT OBJECT SPECTROGRAPH OPTICAL AND ULTRAVIOLET SPECTROSCOPY OF THE BOW SHOCK HH 47A

机译:HH 47A弓形震荡的太空望远镜遥远物体的光谱和紫外光谱

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We present new spectra obtained with the Faint Object Spectrograph aboard the Hubble Space Telescope of the HH 47A bow shock and Mach disk that cover the entire spectral range between λλ2220 and 6810. In addition to emission lines seen previously from HH objects, we uncover over a dozen weak Fe II transitions in the ultraviolet. The flux ratios between these permitted lines can only be understood if transitions to the ground state are resonantly scattered within HH 47A. The expected column density of Fe II within HH 47A suffices to scatter these lines, although the scattering optical depths imply that the Fe II line broadening must exceed that expected from thermal motions. Excitation of ultraviolet Fe II occurs locally within HH 47A, probably from collisions within the hot postshock gas and not from UV pumping from some nearby O stars. The data show no evidence for significant depletion of Fe within HH 47A. The emission line's fluxes and ratios indicate that jet material currently enters the Mach disk with a density of -350 cm~-3 and a velocity of -40 km S~-1. The mass-loss rate of the exciting star, as measured by the mass flux through the Mach disk, is 1.6×10~-)M. Yr~-1. This mass-loss rate is considerably lower than that closer to the star where the jet is brighter, probably because the density along the jet is highly nonuniform. A single-shock velocity does not match the bow shock spectrum well. We propose that secondary shocks reheat the gas within the cooling zone of the HH 47A bow shock. Compression from the first shock will cause these secondary shocks to be str
机译:我们在HH 47A弓形激波和马赫盘的哈勃太空望远镜上用微弱物体光谱仪获得了新的光谱,这些光谱覆盖了λλ2220和6810之间的整个光谱范围。除了先前从HH物体上看到的发射线以外,我们还发现了紫外线中有十几个弱的Fe II过渡。仅当过渡到基态的跃迁在HH 47A中共振散射时,才能理解这些允许线之间的通量比。尽管散射光学深度暗示Fe II线变宽必须超过热运动所预期的宽度,但HH 47A中Fe II的预期柱密度足以散射这些线。紫外线Fe II的激发发生在HH 47A内,可能是由于高温余震气体内部的碰撞所致,而不是来自附近一些O星的紫外线泵激。数据表明,没有证据表明HH 47A中铁的大量消耗。发射线的通量和比率表明射流材料目前以-350 cm〜-3的密度和-40 km S〜-1的速度进入马赫盘。用通过马赫盘的质量通量测得的恒星的质量损失率为1.6×10〜-)M。 Yr〜-1。该质量损失率远低于靠近喷流较亮的恒星的质量损失率,这可能是因为沿喷流的密度非常不均匀。单次冲击的速度与船首的冲击波谱不太匹配。我们建议,二次冲击会在HH 47A弓形冲击的冷却区内重新加热气体。第一次震动的压缩会导致这些二次震动

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