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

机译:观察到的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?

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.udConclusions. 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中性氢组分的直接探针。因此,在红移z = 7.7时测量Lyα发射体的Lyα光度函数(LF),可以使我们在此红移条件下约束宇宙的电离态。方法。我们在VLT处用HAWK-I仪器观察到三个7. 5×7. 5场,其中心为1.06μm的窄带滤光片,并以z 7.7的红移瞄准了Lyα发射器。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,它使我们能够使用引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选择z = 7.7 LAE候选对象,特别是从在光学波段中没有检测到的情况中。结果。我们在z = 7.7的2.4×104 Mpc3的低至AB幅窄至26的窄带中找不到任何LAE候选物,这使我们能够推断出在该红移时对LyαLAE光度函数的鲁棒约束。 ud结论。预测的平均物体数在z = 6.5时,源自Hu等人的发光度函数有些不同。 (2010,ApJ,725,394),Ouchi等。 (2010,ApJ,723,869)和Kashikawa等人。 (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,我们排除了在z = 6.5到z = 7.7之间没有演变的情况,置信度为85%,而无需对IGMLyα透射进行强烈改变,或者在99%置信度下具有显着淬灭可能是由于这两个红移之间的高中性氢比例的强烈增加所致。

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