2025A&A...704A.190R


Query : 2025A&A...704A.190R

2025A&A...704A.190R - Astronomy and Astrophysics, volume 704A190 (2025/12-1)

Optical spectroscopy of blazars for the Cherenkov Telescope Array Observatory - IV.

RAJPUT B., GOLDONI P., MAX-MOERBECK W., KASAI E., WILLIAMS D.A., BOISSON C., PITA S., BACKES M., BARRES DE ALMEIDA U., BECERRA GONZALEZ J., COTTER G., D'AMMANDO F., FALLAH RAMAZANI V., HNATYK B., HERVET O., LINDFORS E., MUKHI-NILO D., NIKOLAJUK M., SPLETTSTOESSER M. and VAN SOELEN B.

Abstract (from CDS):

Context. Blazars, comprising BL Lacertae objects (BL Lacs) and flat-spectrum radio quasars, are the most luminous extragalactic sources that dominate the γ-ray sky. They account for approximately 56% of the sources listed in the recent Fermi-LAT (Large Area Telescope) catalogue (4FGL-DR4). The optical and UV spectra of BL Lacs are nearly featureless, making it difficult to precisely determine their redshifts. Consequently, nearly half of the γ-ray BL Lacs lack reliable redshift measurements. This poses a significant challenge, since redshift is crucial for studying the cosmic evolution of the blazar population and for understanding their intrinsic emission mechanisms. Additionally, it is vital for γ-ray propagation studies, such as indirect evidence of extragalactic background light (EBL), placing constraints on the intergalactic magnetic field (IGMF), and searches for Lorentz invariance violation (LIV) and axion-like particles (ALPs).
Aims. This paper is the fourth in a series dedicated to determining the redshift of a sample of blazars identified as key targets for future observations with the Cherenkov Telescope Array Observatory (CTAO). The precise determination of the redshifts of these objects plays a crucial role in planning future CTAO observations.
Methods. We carried out Monte Carlo simulations to identify potential γ-ray blazars with hard spectra detected by the Fermi-LAT telescope that currently lack redshift measurements. These simulations selected the blazars that are anticipated to be detectable by the CTAO within 30 hours or less of exposure assuming an average flux state. In this fourth paper, we report the results of detailed spectroscopic observations of 29 blazars using the ESO/VLT, Keck II, and SALT telescopes. Our analysis involved a thorough search for spectral lines in the spectra of each blazar, and when features of the host galaxy were identified, we modelled its properties. Moreover, we compared the magnitudes of the targets during the observations to their long-term light curves.
Results. In the sample studied, 9 of 29 sources were observed with a high signal-to-noise ratio (S/N > 100), while the remaining 20 were observed with a moderate or low S/N. We successfully determined firm redshifts for 12 blazars, ranging from 0.1636 to 1.1427, and identified two lower limit redshifts at z > 1.0196 and z > 1.4454. The remaining 15 BL Lac objects exhibited featureless spectra under the observed S/N.

Abstract Copyright: © The Authors 2025

Journal keyword(s): galaxies: active - BL Lacertae objects: general - galaxies: distances and redshifts - gamma rays: galaxies

Simbad objects: 34

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Number of rows : 34
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 1RXS J032342.6-011131 BLL 03 23 43.6189299792 -01 11 46.206256992 17.67 17.48 16.96 17.4   ~ 27 1
2 1FGL J0323.7-0106 mul 03 23 45.3 -01 11 25           ~ 57 0
3 RX J0338.4+1302 BLL 03 38 29.2787338512 +13 02 15.445163688   19.3   18.3   ~ 48 1
4 1RXS J052542.0-601337 BLL 05 25 42.4313688480 -60 13 40.135997408           ~ 40 0
5 1RXS J054030.8+582339 BLL 05 40 30.0094967101 +58 23 38.459367179       16.065   ~ 51 1
6 B2 0557+38 BLL 06 01 02.8707695475 +38 38 29.169121958           ~ 50 1
7 6dFGS gJ062222.1-260545 BLL 06 22 22.0636928064 -26 05 44.639633796   18.57   17.07   ~ 46 0
8 PMN J0622-2605 Rad 06 22 23.73 -26 06 27.6           ~ 16 1
9 NVSS J070242-195123 BLL 07 02 42.90066398 -19 51 22.0355917           ~ 68 1
10 3FGL J0804.0-3629 Bz? 08 04 01.8 -36 29 07           ~ 16 0
11 2MASS J08040532-3629175 BLL 08 04 05.3244075550 -36 29 17.561055761           ~ 4 1
12 RX J0819.2-0756 BLL 08 19 17.5832101176 -07 56 26.141444304       18.4   ~ 43 0
13 PMN J0841-3555 BLL 08 41 21.6333765672 -35 55 05.970173772           ~ 42 1
14 1RXS J094709.2-254056 BLL 09 47 09.5246143707 -25 41 00.028172607           ~ 45 1
15 RX J1055.5-0126 BLL 10 55 34.3694040000 -01 26 16.303689636   18.86 18.54 18.8   ~ 40 0
16 NVSS J123341-014426 BLL 12 33 41.3342161329 -01 44 23.711099800 19.16 18.87 18.46 18.22   ~ 51 0
17 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 3205 2
18 PMN J1307-4259 BLL 13 07 37.9837746648 -42 59 38.986887192 16.39 16.10 15.92 15.80 14.59 ~ 68 1
19 87GB 132042.1+295714 BLL 13 23 02.587 +29 41 33.36   20.7       ~ 68 1
20 2MASS J14403782-3846549 BLL 14 40 37.8231625176 -38 46 54.978605004           ~ 38 0
21 1RXS J154458.3-664153 BLL 15 44 58.9212112900 -66 41 46.840538508           ~ 27 1
22 ICRF J160756.9-203942 BLL 16 07 56.9271636360 -20 39 42.365219400           ~ 36 1
23 1RXS J163750.3-344912 BLL 16 37 50.9780559871 -34 49 16.382917051         16.218 ~ 31 0
24 NVSS J164011+062827 Bz? 16 40 11.0531812988 +06 28 26.965447912           ~ 17 0
25 1RXS J171405.2-202747 BLL 17 14 05.44464 -20 27 52.9362           ~ 34 0
26 ATO J268.5491+32.2064 BLL 17 54 11.7992994912 +32 12 23.055857100           ~ 62 1
27 PMN J1823-3453 BLL 18 23 38.5909469504 -34 54 12.040672189           ~ 56 1
28 1RXS J184919.7-164726 BLL 18 49 19.4661071194 -16 47 23.815576255           ~ 26 1
29 1RXS J192502.7+281540 BL? 19 25 02.2859561131 +28 15 41.204813112           ~ 25 1
30 1RXS J194246.3+103339 BLL 19 42 47.4841298280 +10 33 27.102911688           ~ 63 1
31 1RXS J194422.6-452326 BLL 19 44 22.3904632368 -45 23 32.530725708           ~ 43 1
32 2MASS J19445517-2143190 BLL 19 44 55.1660261454 -21 43 19.323697347           ~ 31 1
33 RX J2247.8+4413 BLL 22 47 53.2057635432 +44 13 15.393598068           ~ 52 1
34 1RXS J230437.1+370506 BLL 23 04 36.7146091872 +37 05 07.422633924     17.50 18.1   ~ 66 0

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