2025MNRAS.540.1308O


Query : 2025MNRAS.540.1308O

2025MNRAS.540.1308O - Mon. Not. R. Astron. Soc., 540, 1308-1328 (2025/June-2)

Optical and near-infrared spectroscopy of quasars at z > 6.5: public data release and composite spectrum.

ONORATO S., HENNAWI J.F., SCHINDLER J.-T., YANG J., WANG F., BARTH A.J., BANADOS E., EILERS A.-C., BOSMAN S.E.I., DAVIES F.B., VENEMANS B.P., MAZZUCCHELLI C., BELLADITTA S., VITO F., FARINA E.P., ANDIKA I.T., FAN X., WALTER F., DECARLI R., ONOUE M. and NANNI R.

Abstract (from CDS):

We present optical and near-infrared (NIR) spectroscopic observations for a sample of 45 quasars at $6.50 < z \le 7.64$ with absolute magnitudes at 1450 Å in the range $-28.82 \le M_{1450} \le -24.13$ and their composite spectrum. The median redshift and $M_{1450}$ of the quasars in the sample are $z_{\rm {median}}=6.71$ and $M_{1450,\rm {median}} \simeq -26.1$, respectively. The NIR spectra are taken with Echelle spectrographs, complemented with additional data from optical long slit instruments, and then reduced consistently using the open-source Python-based spectroscopic data reduction pipeline PypeIt. The median of the mean signal-to-noise ratios per 110 km s$^{-1}$ pixel in the J, H, and K band [median $\langle \rm {SNR}_{\lambda } \rangle$] is median $\langle \rm {SNR}_{J} \rangle =9.7$, median $\langle \rm {SNR}_{H} \rangle =10.3$, and median $\langle \rm {SNR}_{K} \rangle =11.7$; demonstrating the good data quality. This work presents the largest medium-/moderate-resolution sample of quasars at $z>6.5$ from ground-based instruments. Despite the diversity in instrumental set-ups and spectral quality, the data set is uniformly processed and well-characterized, making it ideally suited for several scientific goals, including the study of the quasar proximity zones and damping wings, the Ly $\alpha$ forest, the intergalactic medium's metal content, as well as other properties such as the distribution of SMBH masses and Eddington ratios. Our composite spectrum is compared to others at both high and low z from the literature, showing differences in the strengths of many emission lines, probably due to differences in luminosity among the samples, but a consistent continuum slope, which proves that the same spectral features are preserved in quasars at different redshift ranges.

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

Journal keyword(s): methods: data analysis - techniques: spectroscopic - galaxies: active - quasars: supermassive black holes - cosmology : early Universe

Simbad objects: 72

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Number of rows : 72
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 HSCS J000142+000057 QSO 00 01 42.54 +00 00 57.5           ~ 6 0
2 QSO J0020-3653 QSO 00 20 31.46969 -36 53 41.8114           ~ 25 0
3 QSO J0024+3913 QSO 00 24 29.77000 +39 13 18.9500           ~ 29 0
4 QSO J0038-1527 QSO 00 38 36.09984 -15 27 23.5998           ~ 30 0
5 QSO J0109-3047 QSO 01 09 53.136 -30 47 26.30           ~ 56 0
6 [MOK2016b] HSC J011257.84+011042.4 QSO 01 12 57.84 +01 10 42.4           ~ 5 0
7 [MOK2016b] HSC J021316.94-062615.2 QSO 02 13 16.94 -06 26 15.2           ~ 10 0
8 [MOK2016b] HSC J021430.90+023240.4 QSO 02 14 30.90 +02 32 40.4           ~ 3 0
9 QSO J0218+0007 QSO 02 18 47.04 +00 07 15.0           ~ 14 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 QSO J0229-0808 QSO 02 29 35.25 -08 08 23.0           ~ 2 0
13 QSO J0244-5008 QSO 02 44 01.02 -50 08 53.7           ~ 19 0
14 DES J024655.90-521949.9 QSO 02 46 55.90001 -52 19 49.9001           ~ 9 0
15 QSO J0252-0503 QSO 02 52 16.63999 -05 03 31.7999           ~ 31 0
16 QSO J0305-3150 QSO 03 05 16.918 -31 50 55.85           ~ 102 0
17 QSO J0313-1806 QSO 03 13 43.84 -18 06 36.4           ~ 42 0
18 QSO J0319-1008 QSO 03 19 41.65999 -10 08 46.0000           ~ 12 0
19 VLASS1QLCIR J041009.06-013919.6 Bla 04 10 09.06062 -01 39 19.6683           ~ 6 0
20 VHS J0411-0907 QSO 04 11 28.62984 -09 07 49.8000           ~ 28 0
21 QSO J0430-1445 QSO 04 30 43.66 -14 45 41.2           ~ 2 0
22 [FWY2019] UHS J043947.08+163415.7 QSO 04 39 47.08632 +16 34 16.0140           ~ 59 0
23 QSO J0525-2406 QSO 05 25 59.68 -24 06 23.0           ~ 9 0
24 QSO J0706+2921 QSO 07 06 26.38992 +29 21 05.4997           ~ 10 0
25 DELS J082931.97+411740.4 QSO 08 29 31.96992 +41 17 40.3998           ~ 12 0
26 QSO J0837+4929 QSO 08 37 37.83984 +49 29 00.3998           ~ 14 0
27 DELS J083946.88+390011.5 QSO 08 39 46.87992 +39 00 11.4998           ~ 10 0
28 QSO J0910+1656 QSO 09 10 13.62984 +16 56 29.8000           ~ 14 0
29 [MOK2016b] HSC J091041.14+005646.3 QSO 09 10 41.14 +00 56 46.3           ~ 3 0
30 QSO J0910-0414 QSO 09 10 54.52992 -04 14 06.7999           ~ 13 0
31 [MOK2016b] HSC J091906.33+051235.3 QSO 09 19 06.33 +05 12 35.3           ~ 3 0
32 QSO J0921+0007 QSO 09 21 20.56 +00 07 22.9           ~ 21 0
33 QSO J0923+0402 QSO 09 23 47.12 +04 02 54.4           ~ 26 0
34 [YWF2021] J092359.00+075349.1 QSO 09 23 59.00 +07 53 49.1           ~ 6 0
35 QSO J1007+2115 QSO 10 07 58.26 +21 15 29.2           ~ 39 0
36 [MOK2016b] HSC J103537.74+032435.7 QSO 10 35 37.74 +03 24 35.7           ~ 3 0
37 QSO J1048-0109 QSO 10 48 19.077 -01 09 40.42           ~ 34 0
38 [YWF2021] J105807.72+293041.7 QSO 10 58 07.72 +29 30 41.7           ~ 5 0
39 QSO J1104+2134 QSO 11 04 21.58992 +21 34 28.7998           ~ 18 0
40 PSO J167.6415-13.4960 QSO 11 10 33.963 -13 29 45.73           ~ 45 0
41 [MOK2016b] HSC J111427.15+021517.6 QSO 11 14 27.15 +02 15 17.6           ~ 2 0
42 QSO J1120+0641 QSO 11 20 01.463 +06 41 23.79           ~ 262 0
43 QSO J1129+1846 QSO 11 29 25.34 +18 46 24.2           ~ 32 0
44 [MOK2016b] HSC J113034.65+045013.1 QSO 11 30 34.65 +04 50 13.1           ~ 3 0
45 QSO J1135+5011 QSO 11 35 08.92992 +50 11 32.9996           ~ 11 0
46 QSO J1205-0000 QSO 12 05 05.09 -00 00 27.9           ~ 35 0
47 QSO J1216+4519 QSO 12 16 27.57984 +45 19 10.6997           ~ 13 0
48 HSCS J123137+005230 QSO 12 31 37.77 +00 52 30.3           ~ 5 0
49 HSCS J124353+010038 QSO 12 43 53.93 +01 00 38.5           ~ 23 0
50 [MOK2016b] HSC J131050.13-005054.1 QSO 13 10 50.13 -00 50 54.1           ~ 3 0
51 [MOK2016b] HSC J131746.92+001722.2 QSO 13 17 46.92 +00 17 22.2           ~ 3 0
52 QSO J1342+0928 QSO 13 42 08.100 +09 28 38.36           ~ 145 0
53 [MOK2016b] HSC J134400.87+012827.8 QSO 13 44 00.87 +01 28 27.8           ~ 4 0
54 [MOK2016b] HSC J134905.63+015608.9 QSO 13 49 05.63 +01 56 08.9           ~ 3 0
55 HSCS J142903-010443 QSO 14 29 03.08 -01 04 43.4           ~ 9 0
56 [MOK2016b] HSC J144045.91+001912.9 QSO 14 40 45.91 +00 19 12.9           ~ 3 0
57 [MOK2016b] HSC J145005.39-014438.9 QSO 14 50 05.39 -01 44 38.9           ~ 3 0
58 QSO J1526-2050 QSO 15 26 37.844 -20 50 00.88           ~ 78 0
59 [MOK2016b] HSC J154505.62+423211.6 QSO 15 45 05.62 +42 32 11.6           ~ 8 0
60 HSCS J160953+532821 QSO 16 09 53.03 +53 28 21.0           ~ 4 0
61 HSCS J161207+555919 QSO 16 12 07.12 +55 59 19.2           ~ 4 0
62 [SHB2018] NEPAGN QSO 17 32 43.118 +65 31 13.50           ~ 5 0
63 QSO J2002-3013 QSO 20 02 41.59 -30 13 21.7           ~ 14 0
64 QSO J2102-1458 QSO 21 02 19.21992 -14 58 53.9998           ~ 15 0
65 QSO J2132+1217 QSO 21 32 33.178 +12 17 55.07           ~ 48 0
66 HSCS J221027+030428 QSO 22 10 27.24 +03 04 28.5           ~ 9 0
67 QSO J2211-6320 QSO 22 11 00.60000 -63 20 55.7999           ~ 9 0
68 QSO J2232+2930 QSO 22 32 55.14497 +29 30 32.3136           ~ 42 0
69 [MOK2016b] HSC J225209.17+040243.8 QSO 22 52 09.17 +04 02 43.8           ~ 2 0
70 [YWF2021] J233807.03+214358.2 QSO 23 38 07.03 +21 43 58.2           ~ 4 0
71 QSO J2348-3054 QSO 23 48 33.352 -30 54 10.35           ~ 58 0
72 HSCS J235646+001747 QSO 23 56 46.33 +00 17 47.3           ~ 13 0

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