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HCN AND CO IN THE CENTRAL 630 PARSECS OF THE GALAXY

机译:HCN和CO在银河系中心630处

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Using the QUARRY focal plane array at the FCRAO 14 m, we have mapped the central 630 X 75 pc (l x b = 4.3° x 0.5°) of the Galaxy at ~50″ (2 pc) resolution in both CO and HCN J= 1 → 0 emission. Since HCN emission traces gas with densities approx>100 times larger than that traced by CO, the HCN luminosity measures the mass of dense (n approx> 10~5 cm~(-3)) molecular gas, and the HCN/CO intensity ratio measures gas density. The densest molecular gas is found in the molecular clouds associated with the l = 1.5° complex, Sgr A, Sgr B, and Sgr C. When compared with the Milky Way at the same spatial resolution, the HCN -luminosities in the central kiloparsec of six nearby starburst galactic nuclei are typically larger (factors of ~0.5-20), but the CO luminosities are only moderately larger (factors of ~0.5-5). Averaged over the central 200 pc, the HCN/CO intensity ratio in the starburst galaxies is larger than in the Milky Way, but a few starburst nuclei have similar or smaller HCN/CO intensity ratios when averaged over larger regions. The spatial extent of elevated HCN/CO ratios (approx> 0.08) typically encompasses approx> 200 pc in the starburst galaxies but only ~50 pc in the Milky Way. These results suggest that starburst nuclei have larger masses of dense gas, higher average gas densities in the central 200 pc, and larger regions of enhanced gas density than the Galactic center. When averaged to 630 pc resolution, the HCN and CO spectra show two main velocity components: (1) a broad feature of width ~250 km s~(-1) centered on V_(LSR) = 0 km s~(-1) and (2) a narrow feature of width ~90 km s~(-1) centered on V_(LSR) = 50 km s~(-1). For the broad component, the HCN/CO J = 1 →0 intensity ratio is nearly constant over the entire velocity range, and its small value (R ~ 0.03) is typical of that found in normal galaxies at several kiloparsecs spatial resolution. The gas in the broad velocity component is spatially extended and may represent diffuse molecular gas bound not to individual clouds but rather directly to the Galactic center potential well in a central disk or bar. Gas in the narrow velocity component is associated with the dense giant molecular clouds associated with the l = 1.5° complex, Sgr A, B, and C.
机译:使用FCRAO 14 m处的QUARRY焦平面阵列,我们绘制了中心630 X 75 pc(lxb = 4.3°x 0.5°)在〜50“(2 pc)分辨率下的CO和HCN的J = 1 →0发射。由于HCN排放的痕量气体密度比CO跟踪的气体密度大100倍以上,因此HCN的光度可测量致密(n约> 10〜5 cm〜(-3))分子气体的质量以及HCN / CO强度比测量气体密度。在与l = 1.5°配合物,Sgr A,Sgr B和Sgr C相关的分子云中发现了最稠密的分子气体。当以相同的空间分辨率与银河系进行比较时,位于中央千帕的HCN发光度附近的六个星暴星系核通常较大(约0.5-20的因子),但CO光度仅适度较大(约0.5-5的因子)。在中心200 pc上取平均值,星爆星系中的HCN / CO强度比要比银河系大,但是当在较大区域取平均值时,少数几个星爆核具有相似或较小的HCN / CO强度比。 HCN / CO比值升高的空间范围(约0.08)在星爆星系中通常约200 pc,但在银河系中仅约50 pc。这些结果表明,与银河系中心相比,星爆核具有更大的致密气体质量,中央200 pc的平均气体密度更高,并且气体密度增大的区域更大。当以630 pc分辨率平均时,HCN和CO光谱显示出两个主要速度分量:(1)以V_(LSR)= 0 km s〜(-1)为中心的宽〜250 km s〜(-1)的宽广特征。 (2)以V_(LSR)= 50 km s〜(-1)为中心的宽度〜90 km s〜(-1)的狭窄特征。对于较宽的分量,HCN / CO J = 1→0强度比在整个速度范围内几乎是恒定的,其较小的值(R〜0.03)是几千帕秒空间分辨率下正常星系中的典型值。宽速度分量中的气体在空间上扩展,并且可以表示扩散的分子气体,其不绑定到单个云,而是直接绑定到中央磁盘或条形图中的银河系中心势阱。狭窄速度分量中的气体与与l = 1.5°配合物Sgr A,B和C相关的致密巨型分子云有关。

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