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OB SERVABLE PROPERTIES OF COSMOLOGICAL REIONIZATION SOURCES

机译:宇宙电离源的可观察特性

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Motivated by recent evidence that the epoch of reionization of hydrogen may have ended at a redshift as low as z ≈ 6, we consider the detectability of the sources responsible for this reionization. The main idea is that reionization places limits on the mean surface brightness of the population of reionization sources. Reducing the number of model-dependent assumptions to a minimum, we discuss the observability of these sources with existing and planned telescopes. We define a family of models characterized by two parameters: the Lyman continuum escape fraction f_c from the sources and the dumpiness parameter C of the intergalactic medium. The minimum surface brightness model corresponds to a value of unity for both parameters. We find that the detection of the nonionizing U V continuum of the reionization sources will be difficult to accomplish before the launch of the James Webb Space Telescope (JWST) if these sources have a mean surface brightness close to the minimum value. However, if the values of f_c and C are more realistic, the reionization sources may well be detected by the Hubble Space Telescope before JWST, perhaps by exploiting gravitational lensing amplification by foreground clusters of galaxies. Instead of a detection in the continuum, one may attempt to detect the Lyα emission line by narrowband imaging. Present Lyα searches at z > 6 suggest that either the typical sources are fainter than dwarf galaxies or the escape fraction of ionizing photons is much higher than 50%, so that there are no bright compact H II regions formed around the ionizing sources.
机译:根据最近的证据,氢电离的时代可能以低至z≈6的红移结束了,我们认为是造成这种电离的来源的可检测性。主要思想是,电离会限制电离源总体的平均表面亮度。将与模型有关的假设的数量减少到最少,我们讨论了现有和计划中的望远镜对这些辐射源的可观测性。我们定义了一个以两个参数为特征的模型族:来自源的Lyman连续体逃逸分数f_c和星际介质的矮度参数C。最小表面亮度模型对应于两个参数的单位值。我们发现,如果詹姆斯·韦伯太空望远镜(JWST)发射的平均表面亮度接近最小值,那么将很难完成对这些离子源的非电离U V连续谱的检测。但是,如果f_c和C的值更现实,则可能在JWST之前由哈勃太空望远镜检测到电离源,也许是通过利用星系前景群集的引力透镜放大来实现的。代替连续检测,可以尝试通过窄带成像检测Lyα发射线。目前在z> 6上的Lyα搜索表明,要么典型的源比矮星系更暗,要么电离光子的逸出率远高于50%,因此在电离源周围没有形成明亮的致密H II区。

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