...
首页> 外文期刊>The Astrophysical journal >INTERSTELLAR H2O MASERS FROM J SHOCKS
【24h】

INTERSTELLAR H2O MASERS FROM J SHOCKS

机译:J SHOCKS的星际H2O邮件

获取原文

摘要

We present a model in which the 22?GHz H2O masers observed in star-forming regions occur behind shocks propagating in dense regions (preshock density n 0?~ 106-108?cm–3). We focus on high-velocity (vs 30?km?s–1) dissociative J shocks in which the heat of H2 re-formation maintains a large column of ~300-400?K gas; at these temperatures the chemistry drives a considerable fraction of the oxygen not in CO to form H2O. The H2O column densities, the hydrogen densities, and the warm temperatures produced by these shocks are sufficiently high to enable powerful maser action. The observed brightness temperatures (generally?~ 1011-1014?K) are the result of coherent velocity regions that have dimensions in the shock plane that are 10-100?times the shock thickness of ~1013?cm. The masers are therefore beamed toward the observer, who typically views the shock "edge-on," or perpendicular to the shock velocity; the brightest masers are then observed with the lowest line-of-sight velocities with respect to the ambient gas. We present numerical and analytic studies of the dependence of the maser inversion, the resultant brightness temperature, the maser spot size and shape, the isotropic luminosity, and the maser region magnetic field on the shock parameters and the coherence path length; the overall result is that in galactic H2O 22?GHz masers, these observed parameters can be produced in J shocks with n 0 ~ 106-108?cm–3 and vs ~ 30-200?km?s–1. A?number of key observables such as maser shape, brightness temperature, and global isotropic luminosity depend only on the particle flux into the shock, j = n 0 vs , rather than on n 0 and vs separately.
机译:我们提出了一个模型,其中在恒星形成区域观察到的22?GHz H2O激波发生在密集区域(震前密度n 0?〜106-108?cm-3)中传播的冲击之后。我们专注于高速(vs 30?km?s–1)解离的J冲击,其中H2重组的热量维持着大约300-400?K的大气体柱。在这些温度下,化学物质会驱使CO中的大部分氧气形成H2O。这些冲击产生的H2O柱密度,氢密度和温暖的温度足够高,可以实现强大的maser作用。观测到的亮度温度(通常为?〜1011-1014?K)是相干速度区域的结果,该相干速度区域在冲击平面上的尺寸是冲击厚度约1013?cm的10-100倍。因此,这些激射束朝向观察者发出光束,该观察者通常以“边缘朝上”或垂直于冲击速度的方式观察冲击。然后以相对于环境气体的最低视线速度观察到最亮的脉搏。我们对maser反演,合成亮度温度,maser光斑大小和形状,各向同性光度以及maser区域磁场对冲击参数和相干路径长度的依赖性进行了数值和分析研究;总体结果是,在22?GHz的银河H2O微波激射器中,这些观测到的参数可以在n级为0〜106-108?cm–3和30〜200?km?s–1的J冲击中产生。主要可观测值的数量(例如,maser形状,亮度温度和全局各向同性的光度)仅取决于进入冲击的粒子通量,j = n 0 vs,而不是n 0和vs。

著录项

获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号