论文标题
发现高速h $α$在费米气泡方向的发现
Discovery of High-Velocity H$α$ Emission in the Direction of the Fermi Bubble
论文作者
论文摘要
威斯康星州H-Alpha映射器(WHAM)观察结果揭示了高速度和[NII] $ \ LAMBDA6584 $发射线,沿同一方向和速度与紫外线吸收线相同的方向和速度,这些特征以前曾与已知的Fermi Bubbles已知的双色胶质γ-射线lobes相关。我们测量$ i _ {\ textrm {h}α} = 0.84^{+0.10} _ { - 0.09} $ rayleigh的排放强度的灭绝强度$ v_ \ textrm {lsr} = -221 \ pm3〜 \ textrm {km}〜\ textrm {s}^{ - 1} $,对应于$ em =的排放度量2.00^{+0.64} _ { - 0.63}〜\ textrm {cm}^{ - 6}〜\ textrm {pc} $。这种发射的速度与Hubble空间望远镜/宇宙起源的速度相同,对PDS 456 Quasar瞄准镜在PDS 456类星线中检测到的紫外吸收特征的光谱仪观测值接近$ L = 10^\ Circ.4,B = +11^\ Circ.2 $ 2 $。我们估计该速度组件中电离气体的总柱密度为$ n(h^{+})= \ left(3.28 \ pm 0.33 \ right)\ times 10^{18}〜\ textrm {cm}^{cm}^{ - 2} $。离子气体排放和吸收的比较得出了$ n_ {e,c} = 1.8 \ pm 0.6〜 \ textrm {cm}^{ - 3} $的特征密度的估计值,并且特征长度为$ l_ {c} = 0.56 \ pm pm 0.21〜 \ fextrm $ fectalliant $ pc} $ 30对于$ t_ {e} = 8500^{+2700} _ { - 2600} $ k ---与测量线宽度一致,[nii]/h $α$ line比率---气体的热压为$ p/k = 32,000^{+15,000} _ { - 14,000}〜\ textrm {cm}^{ - 3}〜\ textrm {k} $。假设气体为$ \ sim 6.5 $ kpc距离,则派生的密度和压力似乎异常高的气体$ \ sim $ \ sim 1.3 $ kpc在银河中间平面上方。较大的热压与热光晕或费米气泡模型相当,但建议H $α$在过压的区域中产生。
Wisconsin H-Alpha Mapper (WHAM) observations reveal high-velocity and [NII]$\lambda6584$ emission lines in the same direction and velocity as ultraviolet absorption-line features that have been previously associated with the biconical gamma-ray lobes known as the Fermi Bubbles. We measure an extinction-corrected intensity of $I_{\textrm{H}α}=0.84^{+0.10}_{-0.09}$ Rayleigh for emission with line center $v_\textrm{LSR}=-221\pm3~\textrm{km}~\textrm{s}^{-1}$, corresponding to an emission measure of $EM = 2.00^{+0.64}_{-0.63}~\textrm{cm}^{-6}~\textrm{pc}$. This emission arises at the same velocity as Hubble Space Telescope/Cosmic Origins Spectrograph observations of ultraviolet absorption features detected in the PDS 456 quasar sight line that passes through the northern Bubble near $l = 10^\circ.4, b = +11^\circ.2$. We estimate the total column density of ionized gas in this velocity component to be $N(H^{+}) = \left(3.28 \pm 0.33\right) \times 10^{18}~\textrm{cm}^{-2}$. The comparison of ionized gas emission and absorption yields an estimate for the characteristic density of $n_{e,c} = 1.8 \pm 0.6~\textrm{cm}^{-3}$ and a characteristic length of $L_{c} =0.56 \pm 0.21~\textrm{pc}$ assuming $30\%$ solar metallicity. For a temperature of $T_{e}=8500^{+2700}_{-2600}$ K---consistent with the measured line widths and [NII]/H$α$ line ratio---the gas has a thermal pressure of $p/k = 32,000^{+15,000}_{-14,000}~\textrm{cm}^{-3}~\textrm{K}$. Assuming the gas is $\sim 6.5$ kpc distant, the derived density and pressure appear to be anomalously high for gas $\sim 1.3$ kpc above the Galactic midplane. The large thermal pressure is comparable to both a hot halo or Fermi Bubble model, but suggest that the H$α$ arises in an overpressurized zone.