2026MNRAS.545f1862D


Query : 2026MNRAS.545f1862D

2026MNRAS.545f1862D - Mon. Not. R. Astron. Soc., 545, part no 6, 1862 (2026/January-2)

Updated dark pixel fraction constraints on reionization's end from the Lyman-series forests of XQR-30.

DAVIES F.B., BOSMAN S.E.I., D'ODORICO V., CAMPO S., MESINGER A., QIN Y., BECKER G.D., BANADOS E., CHEN H., CRISTIANI S., FAN X., GALLERANI S., HAEHNELT M.G., KEATING L.C., LAI S., RYAN-WEBER E., WANG F., YANG J. and ZHU Y.

Abstract (from CDS):

The fraction of 'dark pixels' in the Ly$\alpha$ and other Lyman-series forests at $z\sim 5$-6 provides a powerful constraint on the end of the reionization process. Any spectral region showing transmission must be highly ionized, while dark regions could be ionized or neutral, thus the dark pixel fraction provides a (nearly) model independent upper limit to the volume-filling fraction of the neutral intergalactic medium, modulo choices in binning scale and dark pixel definition. Here, we provide updated measurements of the 3.3 comoving Mpc dark pixel fraction at $z=4.85$-6.25 in the Ly$\alpha$, Ly$\beta$, and Ly$\gamma$ forests of 34 deep $5.8 \lesssim z\lesssim 6.6$ quasar spectra from the (enlarged) XQR-30 sample. Using the negative pixel method to measure the dark pixel fraction, we derive fiducial $1\sigma$ upper limits on the volume-average neutral hydrogen fraction of $\langle x_{\rm HI} \rangle \le \lbrace 0.030+0.048,0.095+0.037,0.191+0.056,0.199+0.087\rbrace$ at $\bar{z}=\lbrace 5.481,5.654,5.831,6.043\rbrace$ from the optimally sensitive combination of the Ly$\beta$ and Ly$\gamma$ forests. We further demonstrate an alternative method that treats the forest flux as a mixture of dark and transparent regions, where the latter are modelled using a physically motivated parametric form for the intrinsic opacity distribution. The resulting model-dependent upper limits on $\langle x_{\rm HI} \rangle$ are similar to those derived from our fiducial model-independent analysis. We confirm that the bulk of reionization must be finished at $z>6$, while leaving room for an extended 'soft landing' to the reionization history down to $z\sim 5.4$ suggested by Ly$\alpha$ forest opacity fluctuations.

Abstract Copyright: © The Author(s) 2025. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): intergalactic medium - quasars: absorption lines - dark ages, reionization, first stars - large-scale structure of Universe

Simbad objects: 42

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Number of rows : 42
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 SDSS J002806.57+045725.3 QSO 00 28 06.568 +04 57 25.39           ~ 53 0
2 SDSS J003856.52-102553.8 QSO 00 38 56.519 -10 25 53.97           ~ 32 0
3 SDSS J010013.02+280225.8 QSO 01 00 13.0246669824 +28 02 25.791716364           ~ 206 0
4 SDSS J013201.71-021603.2 QSO 01 32 01.71148560 -02 16 03.2107440           ~ 13 0
5 PSO J025.2376-11.6831 QSO 01 40 57.03 -11 40 59.5           ~ 20 0
6 QSO J0142-3327 QSO 01 42 43.720 -33 27 45.61           ~ 49 0
7 SDSS J014837.63+060020.0 QSO 01 48 37.639 +06 00 20.01           ~ 86 0
8 PSO J029.5172-29.0886 QSO 01 58 04.14 -29 05 19.2           ~ 20 0
9 VST-ATLAS J015957.96-363356.8 QSO 01 59 57.97150 -36 33 56.6028           ~ 29 0
10 VDES J0224-4711 QSO 02 24 26.54 -47 11 29.4           ~ 50 0
11 QSO J0226+0302 QSO 02 26 01.873 +03 02 59.24           ~ 89 0
12 PSO J060.5528+24.8567 QSO 04 02 12.69468 +24 51 24.4284           ~ 30 0
13 VDES J0408-5632 QSO 04 08 19.23 -56 32 28.8           ~ 21 0
14 PSO J065.4085-26.9543 QSO 04 21 38.050 -26 57 15.72           ~ 39 0
15 PSO J065.9589+01.7235 QSO 04 23 50.14129920 +01 43 24.7318320           ~ 15 0
16 [FWY2019] UHS J043947.08+163415.7 QSO 04 39 47.08632 +16 34 16.0140           ~ 59 0
17 PSO J089.9394-15.5833 QSO 05 59 45.46670 -15 35 00.2022           ~ 11 0
18 PSO J108.4429+08.9257 QSO 07 13 46.305984 +08 55 32.65291           ~ 18 0
19 SDSS J081827.40+172251.8 QSO 08 18 27.399 +17 22 51.83   25.14 24.42     ~ 81 0
20 SDSS J083643.85+005453.3 QSO 08 36 43.8598536120 +00 54 53.233681320   26.19 24.17     ~ 170 0
21 SDSS J084229.43+121850.4 QSO 08 42 29.438 +12 18 50.47           ~ 88 0
22 QSO J0923+0402 QSO 09 23 47.12 +04 02 54.4           ~ 26 0
23 SDSS J092721.82+200123.7 QSO 09 27 21.821 +20 01 23.63   24.97 23.89     ~ 79 0
24 SDSS J103027.09+052455.0 QSO 10 30 27.092 +05 24 55.02   26.15 25.44     ~ 303 0
25 PSO J158.6937-14.4210 QSO 10 34 46.49940000 -14 25 15.8924280           ~ 41 0
26 QSO J1212+0505 QSO 12 12 26.97241440 +05 05 33.5606640           ~ 53 0
27 PSO J183.2992-12.7676 QSO 12 13 11.80560 -12 46 03.4464           ~ 24 0
28 SDSS J130608.25+035626.3 QSO 13 06 08.259 +03 56 26.19   25.59 24.81     ~ 176 0
29 SDSS J131911.29+095051.3 QSO 13 19 11.291 +09 50 51.49           ~ 110 0
30 PSO J217.0891-16.0453 QSO 14 28 21.39187 -16 02 43.2990           ~ 33 0
31 PSO J217.9184-07.4120 QSO 14 31 40.447992 -07 24 43.46801           ~ 19 0
32 CFHQS J150941-174926 QSO 15 09 41.77920 -17 49 26.7996           ~ 82 0
33 QSO J1526-2050 QSO 15 26 37.844 -20 50 00.88           ~ 78 0
34 DELS J153532.87+194320.1 QSO 15 35 32.86992 +19 43 20.1000           ~ 23 0
35 PSO J239.7124-07.4027 QSO 15 58 50.990616 -07 24 09.59087           ~ 30 0
36 PSO J242.4396-12.9817 QSO 16 09 45.53040 -12 58 54.1095           ~ 20 0
37 PSO J308.4829-27.6485 QSO 20 33 55.91280 -27 38 54.6000           ~ 21 0
38 QSO J2132+1217 QSO 21 32 33.178 +12 17 55.07           ~ 48 0
39 QSO J2211-3206 QSO 22 11 12.42000 -32 06 12.8002           ~ 30 0
40 VDES J2250-5015 QSO 22 50 02.01 -50 15 42.2           ~ 11 0
41 SDSS J231038.88+185519.7 QSO 23 10 38.888 +18 55 19.72           ~ 107 0
42 SDSS J235632.44-062259.2 QSO 23 56 32.452 -06 22 59.31           ~ 52 0

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