...
首页> 外文期刊>Astronomy and astrophysics >Evolution of the observed Lyα luminosity function from z = 6.5 to z = 7.7: evidence for the epoch of reionization?
【24h】

Evolution of the observed Lyα luminosity function from z = 6.5 to z = 7.7: evidence for the epoch of reionization?

机译:观测到的Lyα光度函数从z = 6.5到z = 7.7的演变:有证据表明电离时代已到来?

获取原文
           

摘要

Aims. Lyα emitters (LAEs) can be detected out to very high redshifts during the epoch of reionization. The evolution of the LAE?luminosity function with redshift is a direct probe of the Lyα transmission of the intergalactic medium (IGM), and therefore of the IGM?neutral-hydrogen fraction. Measuring the Lyα luminosity function (LF) of Lyα emitters at redshift z?=?7.7 therefore allows us to constrain the ionizing state of the Universe at this redshift. Methods. We observed three 7'.5 ?×? 7'.5 fields with the HAWK-I instrument at the VLT with a narrow band filter centred at 1.06 μm and targeting Lyα emitters at redshift z?~?7.7. The fields were chosen for the availability of multiwavelength data. One field is a galaxy cluster, the Bullet Cluster, which allowed us to use gravitational amplification to probe luminosities that are fainter than in the field. The two other fields are subareas of the GOODS Chandra Deep Field South and CFHTLS-D4 deep field. We selected z?=?7.7 LAE candidates from a variety of colour criteria, in particular from the absence of detection in the optical bands. Results. We do not find any LAE candidates at z?=?7.7 in ?~2.4?×?104???Mpc3 down to a narrow band AB magnitude of ?~26, which allows us to infer robust constraints on the Lyα LAE luminosity function at this redshift. Conclusions. The predicted mean number of objects at z?=?6.5, derived from somewhat different luminosity functions of Hu et?al. (2010, ApJ, 725, 394), Ouchi et al. (2010, ApJ, 723, 869), and Kashikawa et al. (2011, ApJ, 734, 119) are 2.5, 13.7, and 11.6, respectively. Depending on which of these luminosity functions we refer to, we exclude a scenario with no evolution from z?=?6.5 to z?=?7.7 at 85% confidence without requiring a strong change in the IGM Lyα transmission, or at 99% confidence with a significant quenching of the IGM Lyα transmission, possibly from a strong increase in the high neutral-hydrogen fraction between these two redshifts.
机译:目的在电离时代,Lyα发射体(LAE)可以检测到非常高的红移。具有红移的LAE发光度函数的演化是银河中间介质(IGM)的Lyα传递的直接探针,因此也是IGM的中性氢组分的直接探针。因此,在红移zα=α7.7处测量Lyα发射体的Lyα发光度函数(LF)可以使我们在该红移条件下约束宇宙的电离态。方法。我们观察到三个7'.5?×?在VLT处使用HAWK-I仪器在7'.5视场中,以1.06μm为中心的窄带滤光片,并将Lyα发射器对准红移z?〜?7.7。选择这些字段是为了获得多波长数据。一个领域是银河团,即子弹团,它使我们能够利用重力放大来探测比该领域更暗的光度。另外两个字段是GOODS Chandra深字段South和CFHTLS-D4深字段的子区域。我们从各种颜色标准中,特别是从在光学带中没有检测到的情况中,选择了z≥0.7的LAE候选物。结果。我们在?〜2.4?×?104 ??? Mpc3中直到z〜= 7.7处没有找到任何LAE候选物,而Mpc3下降到一个窄带AB大小为~~ 26,这使我们可以推断对LyαLAE发光度函数的鲁棒约束。在这个红移。结论。根据Hu等人的发光度函数有些不同,z≥6.5时的预测平均物体数。 (2010,ApJ,725,394),Ouchi等。 (2010,ApJ,723,869)和Kashikawa等(2011,ApJ,734,119)分别是2.5、13.7和11.6。根据我们引用的这些光度函数中的哪一个,我们排除了从z?=?6.5到z?=?7.7没有演变的情况,而置信度为85%,而无需对IGMLyα透射率或置信度为99%进行重大更改。可能是由于这两个红移之间高中性氢比例的强烈增加而导致IGMLyα传递显着淬灭。

相似文献

  • 外文文献
  • 中文文献
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