Lallement R, Snowden S, Kuntz K D, Dame T M, Koutroumpa D, Grenier I, Casandjian J M
GEPI/ Observatoire de Paris, 5 Place Jules Janssen, 92195 Meudon, France.
NASA/GSFC, Greenbelt, MD 20771, USA.
Astron Astrophys Suppl Ser. 2016 Nov;595. doi: 10.1051/0004-6361/201629453. Epub 2016 Nov 17.
Most models identify the X-ray bright North Polar Spur (NPS) with a hot interstellar (IS) bubble in the Sco-Cen star-forming region at ≃130 pc. An opposite view considers the NPS as a distant structure associated with Galactic nuclear outflows. Constraints on the NPS distance can be obtained by comparing the foreground IS gas column inferred from X-ray absorption to the distribution of gas and dust along the line of sight. Absorbing columns towards shadowing molecular clouds simultaneously constrain the CO-H conversion factor.
We derived the columns of X-ray absorbing matter N from spectral fitting of dedicated XMM-Newton observations towards the NPS southern terminus (l ≃ 29°, b ≃ +5 to +11°). The distribution of the IS matter was obtained from absorption lines in stellar spectra, 3D dust maps and emission data, including high spatial resolution CO measurements recorded for this purpose.
N varies from ≃ 4.3 to ≃ 1.3 × 10 cm along the 19 fields. Relationships between X-ray brightness, absorbing column and hardness ratio demonstrate a brightness decrease with latitude governed by increasing absorption. The comparison with absorption data, local and large-scale dust maps rules out a NPS near side closer than 300 pc. The correlation between N and the reddening increases with the sightline length from 300 pc to 4 kpc and is the tightest with Planck -based reddening, suggesting a much larger distance. N(H)/E(B-V) ≃ 4.1 × 10 cm mag, close to Fermi-Planck determinations. N absolute values are compatible with HI-CO clouds at -5 ≤ V ≤ +25 to +45 km s and a NPS potentially far beyond the Local Arm. A shadow cast by a b=+9° molecular cloud constrains X in that direction to ≤ 1.0 × 10 cm K km s. The average X over the fields is ≤ 0.75 × 10 cm K km s.
大多数模型将X射线明亮的北冕环(NPS)与距离约130秒差距的天蝎座-半人马座恒星形成区中的一个热星际(IS)气泡联系起来。另一种观点认为NPS是一个与银河系核外流相关的遥远结构。通过比较从X射线吸收推断出的前景IS气体柱与视线方向上气体和尘埃的分布,可以获得NPS距离的限制。朝向遮蔽分子云的吸收柱同时限制了CO-H转换因子。
我们通过对专门的XMM-牛顿卫星对NPS南端(l≃29°,b≃+5至+11°)的观测进行光谱拟合,得出了X射线吸收物质N的柱密度。IS物质的分布是从恒星光谱中的吸收线、三维尘埃图和发射数据中获得的,包括为此目的记录的高空间分辨率CO测量数据。
沿着19个区域,N从≃4.3×10²¹厘米⁻²变化到≃1.3×10²¹厘米⁻²。X射线亮度、吸收柱和硬度比之间的关系表明,亮度随纬度降低,这是由吸收增加所控制的。与吸收数据、局部和大规模尘埃图的比较排除了NPS近侧距离小于300秒差距的可能性。N与红化之间的相关性随着视线长度从300秒差距增加到4千秒差距而增加,并且与基于普朗克的红化最为紧密,这表明距离要大得多。N(H)/E(B-V)≃4.1×10²¹厘米⁻²/星等,接近费米-普朗克的测定值。N的绝对值与-5≤V≤+25至+45千米/秒的HI-CO云以及一个可能远超出本地旋臂的NPS是兼容的。一个b=+9°分子云投射的阴影将该方向上的X限制在≤1.0×10²¹厘米⁻²·开尔文·千米/秒。这些区域的平均X≤0.75×10²¹厘米⁻²·开尔文·千米/秒。