The extreme faint end of the UV luminosity function at z ∼ 6 through gravitational telescopes: a comprehensive assessment of strong lensing uncertainties

被引:196
作者
Atek, Hakim [1 ]
Richard, Johan [2 ]
Kneib, Jean-Paul [3 ,4 ]
Schaerer, Daniel [5 ]
机构
[1] Sorbonne Univ, CNRS, UMR7095, Inst Astrophys Paris, 98bis Blvd Arago, F-75014 Paris, France
[2] Univ Lyon 1, Univ Lyon, CNRS, Ens Lyon,Ctr Rech Astrophys Lyon,UMR5574, F-69230 St Genis Laval, France
[3] EPFL, Observ Sauverny, Lab Astrophys, CH-1290 Versoix, Switzerland
[4] Aix Marseille Univ, CNRS, LAM, UMR 7326, F-13388 Marseille, France
[5] Univ Geneva, Observ Geneve, 51 Ch Maillettes, CH-1290 Versoix, Switzerland
基金
欧洲研究理事会;
关键词
galaxies: evolution; galaxies: high-redshift; galaxies: luminosity function; gravitational lensing: strong; HUBBLE-FRONTIER-FIELDS; HIGH-REDSHIFT GALAXIES; STAR-FORMING GALAXIES; LOCAL GROUP; MASS; REIONIZATION; POPULATION; EVOLUTION; EPOCH;
D O I
10.1093/mnras/sty1820
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
With the Hubble Frontier Fields program, gravitational lensing has provided a powerful way to extend the study of the ultraviolet luminosity function (LF) of galaxies at z similar to 6 down to unprecedented magnitude limits. At the same time, significant discrepancies between different studies were found at the very faint end of the LF. In an attempt to understand such disagreements, we present a comprehensive assessment of the uncertainties associated with the lensing models and the size distribution of galaxies. We use end-to-end simulations from the source plane to the final LF that account for all lensing effects and systematic uncertainties by comparing several mass models. In addition to the size distribution, the choice of lens model leads to large differences at magnitudes fainter than M-UV = -15 AB mag, where the magnification factor becomes highly uncertain. We perform Markov Chain Monte Carlo (MCMC) simulations that include all these uncertainties at the individual galaxy level to compute the final LF, allowing, in particular, a crossover between magnitude bins. The best LF fit, using a modified Schechter function that allows for a turnover at faint magnitudes, gives a faint-end slope of alpha = -2.01(-0.14)(+0.12), a curvature parameter of beta = 0.48(-0.25)(+0.49), and a turnover magnitude of M-T = -14.93(-0.52)(+0.61). Most importantly, our procedure shows that robust constraints on the LF at magnitudes fainter than M-UV = -15 AB remain unrealistic, as the 95 per cent confidence interval accommodates both a turnover and a steep faint-end slope. More accurate lens modeling and future observations of lensing clusters with the James Webb Space Telescope can reliably extend the ultraviolet (UV) LF to fainter magnitudes.
引用
收藏
页码:5184 / 5195
页数:12
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