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首页> 外文期刊>The Astrophysical journal >THE GAS AND DUST ABUNDANCES OF DIFFUSE HALO CLOUDS IN THE MILKY WAY
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THE GAS AND DUST ABUNDANCES OF DIFFUSE HALO CLOUDS IN THE MILKY WAY

机译:银河中弥散性晕圈的气体和尘埃丰度

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We present Goddard High-Resolution Spectrograph observations of the interstellar Mg II, Si II, P II, S II, Mn II, Cr II, Fe II, Ni II, Zn II, and Ge II lines toward HD 116852, a star at-1.3 kpc from the Galactic plane and a distance of 4.8 kpc in the direction l = 304.9°, b = -16.1°. The intermediate-resolution (FWHM ≈ 11-18 km s~(-1)) observations of these species have S/N ≈ 30-90. The high-resolution (FWHM = 3.5 km s~(-1)) observations of Mn II and Fe II reveal a rich interstellar velocity structure extending from ≈ -70 to +35 km s~(-1). The velocity separation of the absorption components caused by differential Galactic rotation allows us to study the abundances of halo clouds below the Sagittarius and Norma spiral arms. We find that the gas-phase abundances of Mg, Si; S, Mn, Cr, Fe, and Ni relative to Zn in the HD 116852 halo clouds are very similar to those of clouds in the low halo (0.3 ≤ ∣z∣ ≤ 1.5 kpc) toward high-latitude stars in the solar neighborhood. There is a progression toward increasing gas-phase abundance from the Galactic disk to halo. For the entire cloud sample, the average logarithmic gas-phase abundance ratios relative to solar abundance ratios are [Mg/ Zn] = -0.52, [Si/Zn] = -0.26, [S/Zn] = -0.05, [Mn/Zn] = -0.61, [Cr/Zn] = -0.51, [Fe/Zn] = -0.64, and [Ni/Zn] = -0.84. Since Zn is not depleted in the warm neutral gas, these abundance values should be the same as [X/H], There are no systematic differences in these abundances for halo clouds with galactocentric distances ≈7-10 kpc. We find that dust grains contain approximately 70% of the Mg, 45% of the Si, and 77% of the Fe in the halo clouds. The small variation in the halo cloud abundances strongly supports the idea that the cores of the dust grains are resilient and difficult to destroy completely by the processes that circulate gas from the disk to the halo. The gas- and dust-phase abundance patterns in the halo clouds are consistent with more severe grain destruction in the clouds at greater distances from the plane. We calculate (Mg + Fe)/ Si = 3.26 ± 0.64 in the dust grains if solar abundances are used as references and (Mg ± Fe)/Si = 3.91 ± 0.64 if B-star reference abundances are used. These ratios imply that there must be grains composed of Fe-oxides, or perhaps pure Fe, in the halo clouds. Since pure Fe grains are destroyed much more rapidly than silicates behind fast shocks, we favor silicates and oxides as the likely constituents of grain material in the halo clouds.
机译:我们向星系HD 116852(一颗恒星,位于-)处的星际Mg II,Si II,P II,S II,Mn II,Cr II,Fe II,Ni II,Zn II和Ge II线提供戈达德高分辨率光谱仪观测结果。与银河平面相距1.3 kpc,沿方向l = 304.9°,b = -16.1°的距离为4.8 kpc。这些物种的中分辨率(FWHM≈11-18 km s〜(-1))观测值具有S / N≈30-90。对Mn II和Fe II的高分辨率观测(FWHM = 3.5 km s〜(-1))揭示了丰富的星际速度结构,其范围从≈-70到+35 km s〜(-1)。由银河差分旋转引起的吸收分量的速度分离使我们能够研究射手座和诺玛旋臂下方的晕云丰度。我们发现Mg,Si的气相丰度;在HD 116852晕云中,相对于Zn的S,Mn,Cr,Fe和Ni与在太阳附近高纬度恒星中低晕(0.3≤zz≤1.5 kpc)的云非常相似。从银河系盘到晕圈,气相丰度有增加的趋势。对于整个云样本,相对于太阳丰度比的平均对数气相丰度比为[Mg / Zn] = -0.52,[Si / Zn] = -0.26,[S / Zn] = -0.05,[Mn / Zn] =-0.61,[Cr / Zn] =-0.51,[Fe / Zn] =-0.64,和[Ni / Zn] =-0.84。由于未在温暖的中性气体中耗尽Zn,因此这些丰度值应与[X / H]相同。对于半中心距≈7-10 kpc的晕云,这些丰度没有系统上的差异。我们发现,晕云中的尘埃颗粒包含大约70%的Mg,45%的Si和77%的Fe。晕云丰度的微小变化强烈支持以下观点:尘粒的芯具有弹性,并且难以通过将气体从磁盘循环到晕环的过程而完全破坏。晕云中的气相和尘埃相丰度模式与距飞机较远距离的云中更严重的谷物破坏相符。如果使用太阳丰度作为参考,我们计算出尘埃颗粒中的(Mg + Fe)/ Si = 3.26±0.64;如果使用B星参考丰度,则计算为(Mg±Fe)/ Si = 3.91±0.64。这些比率意味着在晕云中必须存在由铁氧化物或纯铁组成的晶粒。由于纯铁晶粒在快速冲击后比硅酸盐的破坏速度要快得多,因此我们首选硅酸盐和氧化物作为晕云中晶粒材料的可能成分。

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