Table 4.
Constraints on the IGM parameters derived using the LOFAR upper limits from Mertens et al. (2025) for the Ar = 0 scenario.
IGM | Credible | z = 8.3 | z = 9.1 | z = 10.1 |
Parameters | intervals | |||
(MCMC | [%] | |||
Model) | ||||
![]() |
68 | [0, 0.15] | [0, 0.13] | [0, 0.2] |
(Single-z) | 95 | [0, 0.57] | [0, 0.55] | [0, 0.47] |
![]() |
68 | [0, 0.24] | [0, 0.06] | [0, 0.01] |
(Joint-z) | 95 | [0, 0.85] | [0, 0.46] | [0, 0.17] |
fheat | 68 | [0, 0.21] | [0, 0.18] | [0, 0.22] |
(Single-z) | 95 | [0, 1] | [0, 0.57] | [0, 0.47] |
fheat | 68 | [0, 0.49] | [0, 0.15] | [0, 0.05] |
(Joint-z) | 95 | [0, 0.9] | [0, 0.54] | [0, 0.21] |
![]() |
68 | [1.8, 7.7] | [2.2, 7.3] | [2.6, 12.8] |
(Single-z) | 95 | [1.8, 50] | [2.2, 21] | [2.6, 22] |
![]() |
68 | [1.8, 28.5] | [2.2, 7.2] | [2.6, 5] |
(Joint-z) | 95 | [1.8, 977] | [2.2, 35.6] | [2.6, 15] |
![]() |
68 | [–300, –124] | [–276, –123] | [–222, –113] |
(Single-z) | 95 | [–345, –23] | [–317, –61] | [–283, –80] |
![]() |
68 | [–264, –4] | [–308, –141] | [–308, –220] |
(Joint-z) | 95 | [–313, 10] | [–337, –36] | [–289., –116] |
![]() |
68 | [0, 26.3] | [0, 28.1] | [0, 20.6] |
(Single-z) | 95 | [0, 56.4.] | [0, 39.5] | [0, 35.5] |
![]() |
68 | [0, 68] | [0, 25] | [0, 14] |
(Joint-z) | 95 | [0, 205] | [0, 41] | [0, 23] |
![]() |
68 | [6, 47] | [9, 46] | [11,38] |
(Single-z) | 95 | [3, 118] | [4, 81] | [3.5, 79] |
![]() |
68 | [0, 135] | [0, 40] | [0, 21] |
(Joint-z) | 95 | [0, 331] | [0, 85] | [0, 33] |
Notes. The first column shows the list of IGM parameters derived from both the Single-z and Joint-z analysis, the second refers to the credible intervals of the disfavoured models, while the last three to the constraints obtained from the analysis at three redshifts.
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