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首页> 外文期刊>The Astrophysical journal >Detection of Ne VIII in the Low-Redshift Warm-Hot Intergalactic Medium*
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Detection of Ne VIII in the Low-Redshift Warm-Hot Intergalactic Medium*

机译:在低红移温热星系间介质中检测Ne VIII *

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High-resolution FUSE and STIS observations of the bright QSO HE 0226-4110 (zem = 0.495) reveal the presence of a multiphase absorption-line system at zabs(O ) = 0.20701 containing absorption from H I (Lyα to Lyθ), C III, O III, O IV, O VI, N III, Ne VIII, Si III, S VI, and possibly S V. Single-component fits to the Ne VIII and O VI absorption doublets yield log N(Ne ) = 13.89 ± 0.11, b = 23 ± 15 km s-1, and v = -7 ± 6 km s-1 and log N(O ) = 14.37 ± 0.03, b = 31 ± 2 km s-1, and v = 0 ± 2 km s-1. The Ne VIII and O VI doublets are detected at 3.9 and 16 σ significance levels, respectively. This represents the first detection of intergalactic Ne VIII, a diagnostic of gas with temperature in the range from ~5 × 105 to ~1 × 106 K. Through the entire absorber, N(Ne )/N(O ) = 0.33 ± 0.10. The O VI and Ne VIII are not likely to have been created in a low-density medium photoionized solely by the extragalactic background at z = 0.2, since the required path length ~11 Mpc (assuming [Z/H] = -0.5) implies that the Hubble flow absorption-line broadening would be ~10 times greater than the observed line widths. A collisional ionization origin is therefore more likely. Assuming [Ne/H] and [O/H] = -0.5, the value N(Ne )/N(O ) = 0.33 ± 0.10 is consistent with gas in collisional ionization equilibrium near T = 5.4 × 105 K with log N(H) = 19.9 and N(H)/N(H ) = 1.7 × 106. Various nonequilibrium ionization processes are also considered, because gas with T ~ (1-6) × 105 K cools efficiently. The observations of O VI and Ne VIII in the z = 0.20701 system support the basic idea that a substantial fraction of the baryonic matter at low redshift exists in hot, very highly ionized gaseous structures. Absorption by the moderately ionized gas (including O IV and S VI) is well modeled by gas in photoionization equilibrium with [Z/H] = -0.5 ± 0.2, log U ~ -1.85, T ~ 2.1 × 104 K, nH ~ 2.6 × 10-5 cm-3, P/k ~ 0.5 cm-3 K, and a path length of ~60 kpc. These values suggest that the moderately ionized absorber may be associated with the modestly enriched photoionized gas in a galaxy group or the outermost regions of a galaxy halo.
机译:明亮的QSO HE 0226-4110(zem = 0.495)的高分辨率FUSE和STIS观察结果表明,在zabs(O)= 0.20701处存在一个多相吸收线系统,其中包含从HI(Lyα到Lyθ),C III, O III,O IV,O VI,N III,Ne VIII,Si III,S VI以及可能的SV。单组分拟合Ne VIII和O VI吸收双峰产生log N(Ne)= 13.89±0.11, b = 23±15 km s-1,v = -7±6 km s-1,log N(O)= 14.37±0.03,b = 31±2 km s-1,v = 0±2 km s -1。 Ne VIII和O VI双重峰分别在3.9和16σ显着水平下检测到。这代表了首次检测到星际Ne VIII,这是对温度范围从〜5×105到〜1×106 K的气体的诊断。在整个吸收器中,N(Ne)/ N(O)= 0.33±0.10。 O VI和Ne VIII不可能仅在z = 0.2时被银河外背景光电离的低密度介质中产生,因为所需的光程约为11 Mpc(假设[Z / H] = -0.5)哈勃流动吸收线的展宽将比观察到的线宽大10倍。因此,碰撞电离起源更有可能。假设[Ne / H]和[O / H] = -0.5,则值N(Ne)/ N(O)= 0.33±0.10与T = 5.4×105 K附近的碰撞电离平衡中的气体一致,log N( H)= 19.9,N(H)/ N(H)= 1.7×106。还考虑了各种非平衡电离过程,因为T〜(1-6)×105 K的气体有效冷却。 z = 0.20701系统中的O VI和Ne VIII的观测结果支持以下基本思想:在低红移下,大部分重质物质存在于热的,高度电离的气态结构中。中度电离的气体(包括O IV和S VI)的吸收在光离子化平衡中被气体很好地模拟,[Z / H] = -0.5±0.2,log U〜-1.85,T〜2.1×104 K,nH〜2.6 ×10-5 cm-3,P / k〜0.5 cm-3 K,路径长度约为60 kpc。这些值表明,适度电离的吸收剂可能与星系组或星系光晕最外层区域中的适度富集的电离气体有关。

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