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首页> 外文期刊>The Astrophysical journal >A DEEP HUBBLE SPACE TELESCOPE SEARCH FOR ESCAPING LYMAN CONTINUUM FLUX AT z ~ 1.3: EVIDENCE FOR AN EVOLVING IONIZING EMISSIVITY*
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A DEEP HUBBLE SPACE TELESCOPE SEARCH FOR ESCAPING LYMAN CONTINUUM FLUX AT z ~ 1.3: EVIDENCE FOR AN EVOLVING IONIZING EMISSIVITY*

机译:在z〜1.3处逃逸lyman连续通量的深层空间望远镜搜索:不断发展的电离发射率的证据*

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We have obtained deep Hubble Space Telescope far-UV images of 15 starburst galaxies at z ~ 1.3 in the GOODS fields to search for escaping Lyman continuum (LyC) photons. These are the deepest far-UV images (m AB = 28.7, 3σ, 1'' diameter) over this large an area (4.83 arcmin2) and provide some of the best escape fraction constraints for any galaxies at any redshift. We do not detect any individual galaxies, with 3σ limits to the LyC (~700 ?) flux 50-149 times fainter (in f ν) than the rest-frame UV (1500 ?) continuum fluxes. Correcting for the mean intergalactic medium (IGM) attenuation (factor ~2), as well as an intrinsic stellar Lyman break (factor ~3), these limits translate to relative escape fraction limits of f esc,rel [0.03, 0.21]. The stacked limit is f esc,rel(3σ) 0.02. We use a Monte Carlo simulation to properly account for the expected distribution of line-of-sight IGM opacities. When including constraints from previous surveys at z ~ 1.3 we find that, at the 95% confidence level, no more than 8% of star-forming galaxies at z ~ 1.3 can have relative escape fractions greater than 0.50. Alternatively, if the majority of galaxies have low, but non-zero, escaping LyC, the escape fraction cannot be more than 0.04. In light of some evidence for strong LyC emission from UV-faint regions of Lyman break galaxies (LBGs) at z ~ 3, we also stack sub-regions of our galaxies with different surface brightnesses and detect no significant LyC flux at the f esc,rel 0.03 level. Both the stacked limits and the limits from the Monte Carlo simulation suggest that the average ionizing emissivity (relative to non-ionizing UV emissivity) at z ~ 1.3 is significantly lower than has been observed in LBGs at z ~ 3. If the ionizing emissivity of star-forming galaxies is in fact increasing with redshift, it would help to explain the high photoionization rates seen in the IGM at z4 and reionization of the IGM at z6.
机译:我们已经在GOODS字段中获得了z〜1.3处15个星爆星系的深哈勃太空望远镜远紫外线图像,以寻找逃逸的莱曼连续体(LyC)光子。这些是在这个大面积(4.83 arcmin2)上最深的远紫外线图像(m AB = 28.7,3σ,直径为1英寸),并为任何红移下的任何星系提供了一些最佳的逃逸分数约束。我们没有检测到任何单独的星系,其LyC(〜700?)通量的3σ极限是弱于静止帧UV(1500?)连续通量的50-149倍(以fν为单位)。校正平均星系间介质(IGM)衰减(因子〜2)以及固有的恒星莱曼断裂(因子〜3),这些限制转化为f esc,rel <[0.03,0.21]的相对逸出分数限制。堆叠极限为f esc,rel(3σ)<0.02。我们使用蒙特卡洛模拟正确地考虑了IGM视线不透明度的预期分布。当包括z〜1.3之前的调查的约束条件时,我们发现,在置信度为95%的情况下,z〜1.3处不超过8%的恒星形成星系的相对逸散率大于0.50。或者,如果大多数星系逃逸的LyC较低但不为零,则逃逸分数不能大于0.04。鉴于一些证据表明,z〜3处的莱曼断裂星系(LBG)的紫外线微弱区域会产生强烈的LyC发射,我们还堆叠了具有不同表面亮度的银河子区域,并且在f esc处未检测到明显的LyC通量, rel <0.03级。堆叠极限和蒙特卡罗模拟的极限都表明,z〜1.3时的平均电离发射率(相对于非电离UV发射率)明显低于LBG在z〜3时的平均电离发射率。形成恒星的星系实际上随着红移而增加,这将有助于解释IGM在z> 4时出现的高电离率和IGM在z> 6时发生的电离。
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