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Table 1.

Overview of the full galaxy sample used in this paper, grouped by C III] and [C II] detection.

ID zsp C III] [C II] Ref.
HZ10 5.657 [†, 1]
COS-3018 6.854 [2, 11]
A383-5.2 6.029 [3, 12]
z7_GND_42912 7.506 [7, 13]
HZ1 5.689 [†, 1]
RXJ 1347-1216 6.766 [†, 14]
GDS3073 5.563 [†, 15]
UVISTA-Z-002 6.634 (a) [†, †]
Himiko 6.595 [4, 8]
CR7 6.604 [9, 10]
CR7a 6.604 [9, 10]
CR7b 6.604 [9, 10]
CR7c 6.604 [9, 10]
COS-13679 7.145 [2, 16]
COS-2987 6.816 [2, 11]
VR7 6.532 [5, 17]
9347 1.851 (b) [†, 6]
6515 1.844 (b) [†, 6]
10076 1.946 (b) [†, 6]
9834 1.764 (b) [†, 6]
9681 1.885 (c) [†, 6]
8490 1.906 (c) [†, 6]

Notes. Spectroscopic redshift is based on the Lyα emission or spectroscopic Lyman break except when otherwise noted.

(a)

Spectroscopic redshift measured from a Gaussian fit to the integrated spectrum of the [C II] line from this work.

(b)

Spectroscopic redshift from the [C II] line emission.

(c)

Spectroscopic redshift from the optical spectra. Typical redshift uncertainties are ΔzLyα ∼ 0.0005 − 0.004, Δz[C II] ∼ 0.0002 − 0.0006, and Δzopt ∼ 0.001. The mark ✓ indicates that the emission line has been detected. The mark ✗ indicates that the emission line has not been detected and an upper limit has been placed on the line flux.

References. C III] and [C II] line references: [†] This work, [1] Capak et al. (2015), [2] Laporte et al. (2017), [3] Stark et al. (2015), [4] Carniani et al. (2018b), [5] Matthee et al. (2017b), [6] Zanella et al. (2018), [7] Hutchison et al. (2019), [8] Zabl et al. (2015), [9] Sobral et al. (2018) [10] Matthee et al. (2017a), [11] Smit et al. (2018), [12] Knudsen et al. (2016), [13] Schaerer et al. (2015), [14] Bradač et al. (2017), [15] Béthermin et al. (2020), [16] Pentericci et al. (2016), [17] Matthee et al. (2019).

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