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A PERVASIVE BROAD COMPONENT IN H I EMISSION LINE PROFILES: TEMPERATURE, TURBULENCE, OR A HELIUM SIGNATURE?

机译:H排放谱中的普遍性广泛成分:温度,湍流或氦信号?

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Gaussian analysis of interstellar neutral hydrogen emission profiles has revealed a pervasive broad component with a width on the order of 34?km?s–1. When present, this component can most readily be identified in high galactic latitude directions where the H I profiles are either intrinsically weak or simple. Examination of published data reveals that this characteristic line width has been found in a variety of other H I features including compact high-velocity clouds, very-high-velocity clouds, and the Magellanic Stream. When its presence is accounted for in the analysis of H I profiles, other families of line widths at 14 and 6?km?s–1 are clearly revealed. Possible mechanisms for producing this broad background component are discussed, including temperature, turbulence, and the critical ionization velocity effect. A line width on the order of 34?km?s–1 would imply a kinetic temperature of 24,000 K, too high to keep the gas neutral; hence it should not be observed in H I emission spectra. Turbulent motions could explain a pervasive broad component, but not why it always has the same numerical value in various classes of H I emission line features. The critical ionization velocity effect hypothesis is intriguing because 34?km?s–1 is the value for helium. Clearly, this could be a coincidence but the other prominent distribution peaks correspond to two families of critical ionization velocities of abundant interstellar elements including C, N, and O (about 14?km?s–1) and metals (about 6?km?s–1). Unfortunately, the mechanism by which this effect operates, even in laboratory situations, is not clearly understood. It is suggested that further investigation of the distribution of H I component line widths by allowing for the existence of a pervasive broad underlying component may cast a clearer light on this intriguing phenomenon.
机译:对星际中性氢排放曲线进行的高斯分析表明,普遍存在的宽分量的宽度约为34?km?s-1。当存在时,该分量最容易在银河系纬度本来就很弱或简单的高银纬度方向上被识别出来。对已发布数据的检查表明,这种特征线宽已在其他多种H I特征中找到,包括紧凑的高速云,超高速云和麦哲伦流。当在H I剖面分析中考虑到它的存在时,在14和6?km?s–1处的其他线宽族被清楚地揭示出来。讨论了产生这种广泛背景成分的可能机制,包括温度,湍流和临界电离速度效应。线宽约34?km?s–1意味着动态温度为24,000 K,太高而无法保持气体中性。因此不应在H I发射光谱中观察到它。湍流运动可以解释无处不在的广义分量,但不能解释为什么它在各种类型的H I发射谱线特征中始终具有相同的数值。临界电离速度效应假设很有趣,因为氦的值是34?km?s-1。显然,这可能是巧合,但其他突出的分布峰对应于丰富的星际元素(包括C,N和O(约14?km?s-1)和金属(约6?km?s-1))的两个临界电离速度族。 s–1)。不幸的是,即使在实验室情况下,这种作用的机理仍不清楚。建议通过允许普遍存在的广泛的下层组分的存在来进一步研究H I组分线宽的分布,可以对该现象产生更清晰的认识。

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