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首页> 外文期刊>The Astrophysical journal >DISCOVERY OF HIGHLY IONIZED HIGH-VELOCITY CLOUDS TOWARD MARKARIAN 509
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DISCOVERY OF HIGHLY IONIZED HIGH-VELOCITY CLOUDS TOWARD MARKARIAN 509

机译:朝向MARKARIAN 509的高度电离的高速云的发现

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We present Goddard High Resolution Spectrograph measurements of the Milky Way halo gas absorption toward Mrk 509 (l = 36.°0, b = -29.°9) in the 1233-1268 and 1521-1558 A spectral regions at a resolution of ≈15 km s~(-1). We detect high-velocity (V_(LSR) ≈ —340 to —170 km s~(-1)) absorption in both members of the C iv λλ1548, 1550 doublet but find no corresponding Si II λ1526 or N V λ1238 absorption. The high-velocity C iv absorption has substructure that can be modeled with two Gaussian components centered at < v_(LSR) > = — 227.5 ± 6.1 and -283.4 ± 3.2 km s~(-1) with N(C IV)/N(Si II) > 1.3 and 5.1 and N(C IV)/N(N V) > 3.0 and 6.6, respectively. To understand the relationship between these highly ionized C IV high-velocity clouds (HVCs) and the more familiar H I HVCs, we obtained sensitive observations of the H I 21 cm emission toward Mrk 509 with the NRAO 140 foot (43 m) telescope. We find no detectable 21 cm emission at the velocities of the C iv HVCs to a 4 σ limit of N(H I) < 4.9 x 10~(17) cm~(-2), but mapping of the 21 cm emission in the area around Mrk 509 indicates that H I HVCs with < v_(LSR)> between —270 and —300 km s~(-1) are located within approximately 1.°5 of the sight line. This suggests that the C IV HVC absorption probes the ionized boundaries of the H I HVCs. Although we cannot completely rule out collisional ionization at T ≥ 10~5 K as a means for producing some of the high-velocity C IV, the observed ionic ratios are sufficiently rigorous for us to reject many collisional ionization models and favor a photoionization interpretation of the ionization structure of the C IV HVCs. A plane-parallel slab model investigated using the photoionization code CLOUDY suggests that the high-velocity C IV absorption can be explained with an almost fully ionized [N(H I)/N(H_(tot)) < 0.01] subsolar metal-licity layer ( ≥ 1 kpc) of low-density gas (≤ 10~(-2) cm~(-3)) photoionized by an extragalactic ionizing background with J_v(Lyman-limit) ~ 10~(-22) ergs cm~(-2) s~(-1) Hz~(-1) sr~(-1). The general properties of the high-velocity C IV absorption more closely resemble those of the high-ionization quasar metal line absorption systems than those of other sight lines through the Milky Way disk and halo.
机译:我们提供戈达德高分辨率光谱仪测量的1233-1268和1521-1558 A光谱区域中朝向Mrk 509(l = 36.°0,b = -29。°9)的银河系晕气的吸收,其分辨率为15公里s〜(-1)。我们在C iv λλ1548、1550 doublet的两个成员中检测到了高速(V_(LSR)≈-340至-170 km s〜(-1))吸收,但未发现相应的Si IIλ1526或N Vλ1238吸收。高速C iv吸收具有可以用两个以 = — 227.5±6.1和-283.4±3.2 km s〜(-1)为中心的高斯分量建模的子结构,其中N(C IV)/ N (Si II)> 1.3和5.1,以及N(C IV)/ N(NV)> 3.0和6.6。为了了解这些高度电离的C IV高速云(HVC)与更熟悉的H I HVC之间的关系,我们使用NRAO 140英尺(43 m)望远镜获得了向Mrk 509的H 21 cm发射的敏感观测结果。我们发现在C iv HVC的速度达到4σ极限N(HI)<4.9 x 10〜(17)cm〜(-2)时没有发现21 cm的发射,但是在该区域映射了21 cm的发射Mrk 509周围的表示具有在-270和-300 km s〜(-1)之间的HI HVC位于视线的大约1.°5之内。这表明C IV HVC吸收探测了H I HVC的离子化边界。尽管我们不能完全排除在T≥10〜5 K时发生碰撞电离作为产生某些高速C IV的方法,但是观察到的离子比率对于我们来说是足够严格的,它可以拒绝许多碰撞电离模型并支持对C IV HVC的电离结构。使用光电离代码CLOUDY研究的平面平行平板模型表明,高速C IV吸收可以用几乎完全电离的[N(HI)/ N(H_(tot))<0.01]次太阳能金属亲和层来解释(≥1 kpc)低密度气体(≤10〜(-2)cm〜(-3))被银河外电离背景以J_v(Lyman-limit)〜10〜(-22)ergs cm〜(- 2)s〜(-1)Hz〜(-1)sr〜(-1)。高速C IV吸收的一般特性比通过银河系圆盘和光环的其他视线更类似于高电离类星体金属线吸收系统。

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