How extinction correction influences the estimate of Lyα escape fraction?

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How extinction correction influences the estimate of Lyα escape fraction? Speaker: Fangxia An (Purple Mountain Observatory; Durham University) fangxiaan@pmo.ac.cn Supervisor: Xianzhong Zheng; Ian Smail; A. Mark Swinbank Collaborator: Xianzhong Zheng (PMO), Cai-Na Hao (TJN), Jia-Sheng Huang (NAO), Xiao-Yang Xia (TJN) (arxiv: 1611.09860, accepted for publication in ApJ)

Outline: ² Background ² Dual Filter: Lyα vs Hα Emitters @ z=2.24 ² The individual @ global Lyα escape fraction at z=2.24 ² The influence of extinction correction

The Cosmic Star Formation History & Narrow-band Imaging Survey Lyα1216Å z = 2.25 Madau & Dickinson (2014) 50% of local stars were formed before z~1.3, 25% before z~2, 25% after z~0.7, <1% before z>6. Narrow-band imaging survey 1) Emission-line Objects 2) Large sky coverage 3) δz/(1 + z) = 1 2%

How Lyα is Produced and Escaped from Galaxies HII Produce: Emitted by hot, young star HI HII; Improtance: 1. Galaxies properties: SFR, Dust attenuation, etc. HI 2. Extensive: Lyα: (1216 Å): Lyα has been successfully used to find galaxies across redshifts z 2 7,even probing the end of the epoch of reionization. 3. The amount of ionizing photons: ξ ion =Q ion /L UV,int Q ion Q ion =L Lyα /c Lyα (1-f esc ) Escape: 1. Lyα: (1216 Å) dust absorbing; 2. Lyα photons resonantly scatter on neutral HI gas.

Lyα escape fraction Lyα/Hα HII HI Lyα: Emitted by hot, young star strong & physics of star formation; Resonant nature distribution, Kinematics of a galaxy's ISM (HI); Dust absorption. Hα: Same production mechanism as that of Lyα; Non-resonant recombination line (in Case B recombination: intrinsic Lyα/Hα=8.7 ); Less sensitive to dust.

Dual Filter: Lyα vs Hα Emitters @z=2.24 J.-S. Huang (PI) Telescope: 6.5m Magellan/Megacam Custom-made Filter: NB393(3928Å) Coverage: 25 x 25 Fields: CDFS & COSMOS X.Z. Zheng (PI) Telescope: 3.6m CFHT/WIRCam Filter: H 2 S1 (2.13μm) Coverage: 20 x 20 Fields: CDFS

Sample selection CFHT/WIRCam AB=22.8 (5σ) 56 Hα emitters Magellan/Megacam AB=26.4 (5σ) 124/241 Lyα emitters An, F. X., Zheng, X. Z., et al. 2014, ApJ, 784,152 4 both lines (LAHAEs) An, F. X., et al. arxiv:1611.09860

LAHAEs in COSMOS 2.206< z < 2.312 2.216< z < 2.248 Sobral +13 Vega=22.0 (5σ) Nilsson +09 AB=25.3 (5σ) 158 Hα emitters 146 Lyα emitters 7 both lines

How extinction correction affect the estimate of Individual Lyα escape fraction? Extinction Correction in An+14: Calzetti extinction law (Calzetti + 00 ) with the assumption of E(B-V)cont = 0.4E(B-V)nebu Erb+06 E(B-V)cont = E(B-V)nebu

How extinction correction affect the estimate of Individual Lyα escape fraction? Wuyts+13 Reddy +15 Extinction Correction in this work: Cardelli Galactic extinction law (Cardelli+89 ) with the assumption: A extra =0.9A cont - 0.15A 2 cont Lyα: E(B-V)nebu This work κ Hα (Cardelli) κ Hα (Calzetti00) (< 0.01 mag) κ Lyα (Cardelli) = 1.7 κ Lyα (Calzetti00)

How extinction correction affect the estimate of Individual Lyα escape fraction? 1. A higher intrinsic Lyα/Hα than case B: 1):more complicated geometry and kinematics of the H I region; (e.g., Song14) 2) collisional excitation by shock from AGN or supernovaderived winds 1/3 of LAHAEs are AGNs 2. Uncertainties caused by extinction correction: 1) dust attenuation curve at high-z is correlated with stellar mass (Zeimann15) 2) the large scatter between E(B-V)nebu and E(B-V)cont

Correction between Lyα escape fraction and dust attenuation f esp =L obs (Lyα)/(8.7L int (Hα)) 1. An anti-correlation between Lyα escape fraction and dust attenuation is found. f esp = C Lyα 10-0.4E(B-V) κlyα 2. The resonant scatter on the neutral HI gas can contribute to more than half of the suppression of Lyα escape. 3. E(B-V) nebu vs E(B- V) cont : ~3 percentage points in individual Lyα escape fraction.

How extinction correction affect the estimate of Volumetric Lyα escape fraction? fv esp =ρ obs (L Lyα )/(8.7 ρ int (L Hα )) =(3.7± 1.4)% (A nebu -corrected) 1. Independence on cosmic variance, the evolutionary state of the galaxies, or calibration uncertainties; 2. This method is sensitive to the extinction correction. A cont -corrected: (2.8± 1.2)% The different assumption of E(B-V) nebu cause a deviation of 1 percentage point.

Summary n The different assumption of nebular color excess will cause a discrepancy of up to ~3 percentage points in individual Lyα escape fraction; n The Hα sample show an anti-correction of f esp with dust content; n The global Lyα escape fraction is ~4% at z=2.24 in ECDFS. The variation in the nebular color excess of extinction leads to a discrepancy of ~1 percentage point. Extinction correction significantly influence the estimate of both individual and global individual Lyα escape fraction!

Thanks for your attention! Comments and Questions are Welcome!

Properties of LAHAEs -1 LHα=42.63 erg s -1 LLyα=42.20 erg s Av=2.35 mag Log M/M = 10.75 Mergers/Close pairs -1 LHα=42.80 erg s LLyα=43.08-1 erg s Av=2.16 mag Log M/M = 11.14 Compact X-ray -1 LHα=42.47 erg s -1 LLyα=43.08 erg s Av=0.003 mag Log M/M = 9.35 Mergers/Close pairs -1 LHα=42.29 erg s -1 LLyα=42.36 erg s Av=0.51 mag Log M/M = 9.26 Mergers/Close pairs

Why only few galaxies in both lines? So few Hα emitter are detected in Lyα: 1. κ1216(lyα) = 20 while κ6563(hα) = 3.3 (Cardelli Galactic extinction law); 2. Resonant scattering of Lyα. So few Lyα emitter are detected in Hα: Lyα selection preferentially finds galaxies with high f esc and small attenuation in Hα, resulting in line ratios nearernthe recomination value and comparatively faint Hα.