Open Access
Table D.1.
Non-exhaustive compilation of α measurements for [O III], Hβ, Hα and UV LFs.
| Paper | Redshift | Tracer | Par. | α |
|---|---|---|---|---|
| Sobral et al. (2013) | 0.40 | Hα | SCH | ![]() |
| 0.84 | Hα | SCH | ![]() |
|
| 1.47 | Hα | SCH | ![]() |
|
| 2.23 | Hα | SCH | ![]() |
|
| Colbert et al. (2013) | 0.60 | Hα | SCH | ![]() |
| 1.20 | Hα | SCH | ![]() |
|
| Hayashi et al. (2018) | 0.25 | Hα | SCH | ![]() |
| 0.40 | Hα | SCH | ![]() |
|
| Khostovan et al. (2020) | 0.47 | Hα | SCH | ![]() |
| Nagaraj et al. (2023) | 1.36 | Hα + [N II] | SCH | ![]() |
| Bollo et al. (2023) | 4.50 | Hα | SCH | ![]() |
| Covelo-Paz et al. (2025) | 4.45 | Hα | SCH | ![]() |
| 5.30 | Hα | SCH | ![]() |
|
| 6.15 | Hα | SCH | ![]() |
|
| Fu et al. (2025) | 4.50 | Hα | SCH | ![]() |
| 6.30 | Hα | SCH | ![]() |
|
| Colbert et al. (2013) | 1.10 | [O III] | SCH | ![]() |
| 1.90 | [O III] | SCH | ![]() |
|
| Hayashi et al. (2018) | 0.63 | [O III] | SCH | ![]() |
| 0.84 | [O III] | SCH | ![]() |
|
| Khostovan et al. (2020) | 0.93 | [O III] | SCH | ![]() |
| Bongiovanni et al. (2020) | 0.83 | [O III] | SCH | ![]() |
| Bowman et al. (2021) | 2.12 | [O III] | SCH | ![]() |
| Nagaraj et al. (2023) | 1.53 | [O III]λ5008 | SCH | ![]() |
| Wold et al. (2025) | 7.00 | [O III]λ5008 | DPL | ![]() |
| Reddy & Steidel (2009) | 2.30 | UV | SCH | ![]() |
| 3.05 | UV | SCH | ![]() |
|
| Parsa et al. (2016) | 1.70 | UV | SCH | ![]() |
| 1.90 | UV | SCH | ![]() |
|
| 2.25 | UV | SCH | ![]() |
|
| 2.80 | UV | SCH | ![]() |
|
| 3.80 | UV | SCH | ![]() |
|
| Atek et al. (2018) | 6.00 | UV | SCH | ![]() |
| Moutard et al. (2020) | 0.17 | UV | SCH | ![]() |
| 0.38 | UV | SCH | ![]() |
|
| 0.53 | UV | SCH | ![]() |
|
| 0.75 | UV | SCH | ![]() |
|
| 1.10 | UV | SCH | ![]() |
|
| 1.55 | UV | SCH | ![]() |
|
| Bowler et al. (2020) | 8.00 | UV | SCH | ![]() |
| 9.00 | UV | SCH | ![]() |
|
| Bowler et al. (2020) | 8.00 | UV | DPL | ![]() |
| Bouwens et al. (2022) | 2.00 | UV | SCH | ![]() |
| 3.00 | UV | SCH | ![]() |
|
| 4.00 | UV | SCH | ![]() |
|
| 5.00 | UV | SCH | ![]() |
|
| 6.00 | UV | SCH | ![]() |
|
| 7.00 | UV | SCH | ![]() |
|
| 8.00 | UV | SCH | ![]() |
|
| 9.00 | UV | SCH | ![]() |
|
| Donnan et al. (2023) | 8.00 | UV | DPL | ![]() |
| Harikane et al. (2024) | 7.00 | UV | SCH | ![]() |
| 8.00 | UV | SCH | ![]() |
|
| Harikane et al. (2024) | 7.00 | UV | DPL | ![]() |
| 8.00 | UV | DPL | ![]() |
|
| Donnan et al. (2024) | 9.00 | UV | DPL | ![]() |
| 10.00 | UV | DPL | ![]() |
|
| 11.00 | UV | DPL | ![]() |
|
| Sun et al. (2024) | 0.70 | UV | SCH | ![]() |
| 0.90 | UV | SCH | ![]() |
|
| Willott et al. (2024) | 8.00 | UV | SCH | ![]() |
| Finkelstein et al. (2024) | 9.00 | UV | DPL | ![]() |
| 11.00 | UV | DPL | ![]() |
|
| 14.00 | UV | DPL | ![]() |
|
| Chemerynska et al. (2026) | 9.50 | UV | DPL | ![]() |
| 10.50 | UV | DPL | ![]() |
|
| 11.50 | UV | DPL | ![]() |
|
| 13.00 | UV | DPL | ![]() |
|
| Weibel et al. (2025) | 10.00 | UV | DPL | ![]() |
Notes. Two parametrisations are considered: the most common is the Schechter function (SCH), but we also report the use of double power law (DPL) in a few studies. The data is shown in Fig. 8.
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