2024A&A...688A.106N


Query : 2024A&A...688A.106N

2024A&A...688A.106N - Astronomy and Astrophysics, volume 688A106 (2024/8-1)

Peering into cosmic reionization: Lyα visibility evolution from galaxies at z = 4.5-8.5 with JWST.

NAPOLITANO L., PENTERICCI L., SANTINI P., CALABRO A., MASCIA S., LLERENA M., CASTELLANO M., DICKINSON M., FINKELSTEIN S.L., AMORIN R., ARRABAL HARO P., BAGLEY M., BHATAWDEKAR R., CLERI N.J., DAVIS K., GARDNER J.P., GAWISER E., GIAVALISCO M., HATHI N., HOLWERDA B.W., HU W., JUNG I., KARTALTEPE J.S., KOEKEMOER A.M., LARSON R.L., MERLIN E., MOBASHER B., PAPOVICH C., PARK H., PIRZKAL N., TRUMP J.R., WILKINS S.M. and YUNG L.Y.A.

Abstract (from CDS):

The resonant scattering interaction between Lyα photons and neutral hydrogen implies that a partially neutral intergalactic medium has the ability to significantly impact the detectability of Lyα emission in galaxies. Thus, the redshift evolution of the Lyα equivalent width distribution of galaxies offers a key observational probe of the degree of ionization during the Epoch of Reionization (EoR). Previous in-depth investigations at z ≥ 7 were limited by ground-based instrument capabilities. We present an extensive study of the evolution of Lyα emission from galaxies at 4.5 < z < 8.5, observed as part of the CEERS and JADES surveys in the JWST NIRSpec/PRISM configuration. The sample consists of 235 galaxies in the redshift range of 4.1 < z < 9.9. We identified 65 of them as Lyα emitters. We first measured the Lyα escape fractions from Lyα to Balmer line flux ratios and explored the correlations with the inferred galaxies' physical properties, which are similar to those found at lower redshift. We also investigated the possible connection between the escape of Lyα photons and the inferred escape fractions of LyC photons obtained from indirect indicators, finding no secure correlation. We then analyzed the redshift evolution of the Lyα emitter fraction, finding lower average values at z = 5 and 6 compared to previous ground-based observations. At z = 7, the GOODS-S results are aligned with previous findings, whereas the visibility in the EGS field appears to be enhanced. This discrepancy in Lyα visibility between the two fields could potentially be attributed to the presence of early reionized regions in the EGS. Such a broad variance is also expected in the Cosmic Dawn II radiation-hydrodynamical simulation. The average Lyα emitter fraction obtained from the CEERS+JADES data continues to increase from z = 5 to 7, ultimately declining at z = 8. This suggests a scenario in which the ending phase of the EoR is characterized by ∼1 pMpc ionized bubbles around a high fraction of moderately bright galaxies. Finally, we characterize such two ionized regions found in the EGS at z = 7.18 and z = 7.49 by estimating the radius of the ionized bubble that each of the spectroscopically-confirmed members could have created.

Abstract Copyright: © The Authors 2024

Journal keyword(s): galaxies: evolution - galaxies: high-redshift - intergalactic medium - galaxies: ISM - dark ages - reionization - first stars

Simbad objects: 53

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Number of rows : 53
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 ACO 2744 ClG 00 14 20.03 -30 23 17.8           ~ 1077 0
2 NAME GOODS Southern Field reg 03 32 28.0 -27 48 30           ~ 1623 1
3 [ADF2023] CEERS MSA 82043 EmG 14 18 52.7966 +52 45 00.918           ~ 2 0
4 [ADF2023] CEERS MSA 82069 EmG 14 18 55.277 +52 45 17.90           ~ 3 0
5 [ADF2023] CEERS MSA 82171 EmG 14 18 57.972 +52 44 09.65           ~ 1 0
6 NAME Extended Groth Strip reg 14 19 +52.8           ~ 1023 0
7 CANDELS EGS F160W J141901.9+524559.4 EmG 14 19 01.924 +52 45 59.39           ~ 4 0
8 CANDELS EGS F160W J141904.4+524303.5 EmG 14 19 04.405 +52 43 03.53           ~ 5 0
9 [ADF2023] CEERS MSA 80596 EmG 14 19 05.2476 +52 46 41.480           ~ 2 0
10 [ADF2023] CEERS MSA 80573 EmG 14 19 05.7418 +52 46 50.156           ~ 3 0
11 [ADF2023] CEERS MSA 81049 EmG 14 19 09.5573 +52 43 50.840           ~ 5 0
12 CANDELS EGS F160W J141911.0+524257.2 EmG 14 19 11.040 +52 42 57.19           ~ 4 0
13 [ADF2023] CEERS MSA 476 EmG 14 19 13.335 +52 50 10.84           ~ 2 0
14 [ADF2023] CEERS MSA 355 EmG 14 19 13.5557 +52 52 43.777           ~ 8 0
15 [ADF2023] CEERS MSA 81026 EmG 14 19 14.3618 +52 45 15.185           ~ 2 0
16 [ADF2023] CEERS MSA 80432 EmG 14 19 14.8934 +52 44 48.289           ~ 7 0
17 CANDELS EGS F160W J141915.1+525003.3 EmG 14 19 15.129 +52 50 03.33           ~ 12 0
18 [ADF2023] CEERS MSA 83764 EmG 14 19 15.673 +52 45 20.16           ~ 1 0
19 [ADF2023] CEERS MSA 83779 EmG 14 19 17.1401 +52 45 17.417           ~ 2 0
20 CANDELS EGS F160W J141917.9+525044.7 EmG 14 19 17.90 +52 50 44.8           ~ 5 0
21 [ADF2023] CEERS MSA 439 EmG 14 19 18.0874 +52 51 47.034           ~ 6 0
22 [ADF2023] CEERS MSA 20 EmG 14 19 19.364 +52 53 15.98           ~ 14 0
23 [ADF2023] CEERS MSA 80445 EmG 14 19 22.3476 +52 44 52.390           ~ 5 0
24 CANDELS EGS F160W J141926.2+525113.0 EmG 14 19 26.20 +52 51 13.1           ~ 10 0
25 CANDELS EGS F160W J141926.3+525316.7 EmG 14 19 26.30 +52 53 17.1           ~ 5 0
26 [ADF2023] CEERS MSA 829 EmG 14 19 26.7825 +52 52 34.172           ~ 5 0
27 [ADF2023] CEERS MSA 603 EmG 14 19 28.1393 +52 50 12.253           ~ 6 0
28 [ADF2023] CEERS MSA 323 EmG 14 19 29.4134 +52 52 33.416           ~ 7 0
29 [ADF2023] CEERS MSA 80072 EmG 14 19 33.8040 +52 48 50.188           ~ 2 0
30 [ADF2023] CEERS MSA 80916 EmG 14 19 33.9912 +52 48 57.395           ~ 4 0
31 [ADF2023] CEERS MSA 80239 EmG 14 19 35.0530 +52 52 11.471           ~ 5 0
32 [ADF2023] CEERS MSA 80374 EmG 14 19 35.5378 +52 49 29.622           ~ 5 0
33 [ADF2023] CEERS MSA 83502 EmG 14 19 37.4033 +52 48 42.862           ~ 2 0
34 [ADF2023] CEERS MSA 80944 EmG 14 19 40.090 +52 49 02.90           ~ 1 0
35 [ADF2023] CEERS MSA 82372 EmG 14 19 41.907 +52 52 07.84           ~ 1 0
36 [ADF2023] CEERS MSA 80372 EmG 14 19 42.6715 +52 51 00.011           ~ 4 0
37 CANDELS EGS F160W J141946.5+525100.3 EmG 14 19 46.529 +52 51 00.26           ~ 9 0
38 [ADF2023] CEERS MSA 80925 EmG 14 19 47.683 +52 51 11.78           ~ 3 0
39 CANDELS EGS F160W J141957.3+525953.0 EmG 14 19 57.299 +52 59 53.00           ~ 6 0
40 CANDELS EGS F160W J141959.8+525823.9 EmG 14 19 59.808 +52 58 23.89           ~ 4 0
41 [ADF2023] CEERS MSA 44 EmG 14 20 00.2676 +53 00 40.568           ~ 9 0
42 CANDELS EGS F160W J142005.5+525728.0 EmG 14 20 05.484 +52 57 28.00           ~ 3 0
43 CANDELS EGS F160W J142013.8+525937.4 EmG 14 20 13.804 +52 59 37.36           ~ 3 0
44 [ADF2023] CEERS MSA 1142 EmG 14 20 14.579 +52 57 31.56           ~ 5 0
45 CANDELS EGS F160W J142019.2+525724.4 EmG 14 20 19.210 +52 57 24.44           ~ 7 0
46 CANDELS EGS F160W J142022.3+525738.5 EmG 14 20 22.28 +52 57 38.6           ~ 5 0
47 CANDELS EGS F160W J142027.9+525827.1 EmG 14 20 27.866 +52 58 27.10           ~ 5 0
48 [ADF2023] CEERS MSA 1414 EmG 14 20 30.725 +52 59 05.83           ~ 5 0
49 [LOQ2022] EGSY-23959 EmG 14 20 36.211 +52 59 22.45           ~ 10 0
50 CANDELS EGS F160W J142036.6+530325.4 EmG 14 20 36.632 +53 03 25.40           ~ 7 0
51 CANDELS EGS F160W J142039.9+530414.7 EmG 14 20 39.87 +53 04 14.9           ~ 10 0
52 CANDELS EGS F160W J142040.6+530317.2 EmG 14 20 40.610 +53 03 17.20           ~ 6 0
53 CANDELS EGS F160W J142041.5+530208.9 EmG 14 20 41.461 +53 02 08.89           ~ 5 0

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