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ALMA hints at the existence of an unseen reservoir of diffuse molecular gas in the Galactic bulge

机译:Alma暗示在银河膨胀中的弥漫分子气体的看不见的储层

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Aims. We aim to understand the unexpected presence of mm-wave molecular absorption at ? 200 km?s ~(-1) & v & ?140 km?s ~(-1) in a direction that is well away from regions of the Galactic bulge where CO emission at such velocities is prominent. Methods. We compared 89 GHz Cycle 2 ALMA absorption spectra of HCO ~(+) , HCN, and HNC toward the extragalactic continuum source B1741-312 at l = ? 2.14 ° , b = ? 1.00 ° with existing CO, H I, and dust emission and absorption measurements. We placed the atomic and molecular gas in the bulge and disk using circular and non-circular galactic kinematics, deriving N (H I) from a combination of 21 cm emission and absorption and we derive N ( H_(2) ) from scaling of the HCO ~(+) absorption. We then inverted the variation of near-IR reddening E ( J ? K ) with distance modulus and scale E ( J ? K ) to a total gas column density N (H) that may be compared to N (H I) and N ( H_(2) ). Results. At galactocentric radii R _(gal) & 1.5 kpc, conventional measures such as the standard CO- H_(2) conversion factor and locally observed N (HCO ~(+) )/ N ( H_(2) ) ratio separately imply that H I and H_(2) contribute about equally to N (H), and the gas-derived N (H) values are in broad agreement with those derived from E ( J ? K ) . Within the Galactic bulge at R _(gal) & 1.5 kpc, H I contributes less than 10% of the material inferred from E ( J ? K ) , so that the molecular absorption detected here is needed to understand the extinction.
机译:目标。我们的目标是理解MM波分子吸收的意外存在? 200 km?s〜(-1)& v& ?140 km?s〜(-1)在远离银河凸起的区域的方向上,在这种速度下的共同发射是突出的。方法。我们将HCO〜(+),HCN和HNC的89 GHz循环2 Alma吸收光谱与L =Δ相比,朝向紫外线源B1741-312进行比较。 2.14°,B =? 1.00°具有现有的CO,H I和灰尘发射和吸收测量。我们使用圆形和非圆形银河气相学置于凸起和盘中的原子和分子气体,从21cm发射和吸收的组合衍生N(HI),我们从HCO的缩放中获得N(H_(2)) 〜(+)吸收。然后,我们将近红外变红e(j×k)的变化与距离模量和尺寸e(j≤k)倒到的总气柱密度n(h),其可以与n(hi)和n(h_)进行比较(2))。结果。在Galactocentric Radii R _(GAL)> 1.5 KPC,诸如标准CO-H_(2)转换因子和本地观察到的N(HCO〜(+))/ N(H_(2))比例的常规测量分别意味着HI和H_(2)截然达到N(H),气体衍生的N(H)值与来自e(j'k k)的那些达成广泛的协议。在R _(GAL)< 1.5 kPc,h i贡献从e(j?k)推断的少于10%的材料,从而需要在此检测到的分子吸收来理解灭绝。

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