2023ApJ...943L..18C


Query : 2023ApJ...943L..18C

2023ApJ...943L..18C - Astrophys. J., 943, L18 (2023/February-1)

Linear and Circular Polarimetry of the Optically Bright Relativistic Tidal Disruption Event AT 2022cmc.

CIKOTA A., LELOUDAS G., BULLA M., DAI L., MAUND J. and ANDREONI I.

Abstract (from CDS):

Tidal disruption events (TDEs) occur when a star orbiting a massive black hole is sufficiently close to being tidally ripped apart by the black hole. AT 2022cmc is the first relativistic TDE that was observed (and discovered) as an optically bright and fast transient, showing signatures of nonthermal radiation induced by a jet that is oriented toward the Earth. In this work, we present optical linear and circular polarization measurements, observed with the Very Large Telescope/FORS2 in the R band (which corresponds to the blue/UV part of the spectrum in the rest frame), ∼7.2 and ∼12.2 rest-frame days after the first detection, respectively, when the light curve of the transient had settled in a bright blue plateau. Both linear and circular polarizations are consistent with zero, plin = 0.14% ± 0.73%, and pcir = -0.30% ± 0.53%. This is the highest signal-to-noise ratio linear polarization measurement obtained for a relativistic TDE and the first circular polarimetry for such a transient. The nondetection of the linear and circular polarizations is consistent with the scenario of AT 2022cmc being a TDE where the thermal component (disk+outflows) is viewed pole-on, assuming an axially symmetric geometry. The presence and effect of a jet and/or external shocks are, however, difficult to disentangle.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Tidal disruption - Polarimetry - High energy astrophysics - Relativistic jets

Simbad objects: 16

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Number of rows : 16
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 AT 2020mot ev 00 31 13.560 +85 00 31.90           ~ 28 0
2 2MASS J01580475-0052221 Sy1 01 58 04.7506373016 -00 52 21.927742716   18.84 18.34     SNII 114 1
3 GRB 121024A gB 04 41 53.31 -12 17 26.1           ~ 143 0
4 AT 2019qiz ev 04 46 37.880 -10 13 34.92           ~ 143 0
5 Z 119-12 SyG 08 13 16.9505119752 +22 38 53.905852212           ~ 156 0
6 SWIFT J1112.2-8238 X 11 11 47.797 -82 38 44.71           ~ 81 0
7 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 3205 2
8 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
9 AT 2022cmc ev 13 34 43.207 +33 13 00.54           ~ 79 0
10 QSO J1512-0906 Bla 15 12 50.53293048 -09 05 59.8297908   16.74 16.54     ~ 1409 1
11 2MASX J16105891-6055250 AG? 16 10 58.8863559654 -60 55 24.411688282           ~ 78 0
12 SN 2018cow SN* 16 16 00.254 +22 16 05.10           SNIb 305 0
13 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
14 2MASX J20570298+1412165 G 20 57 02.9650698480 +14 12 16.295014080           ~ 162 0
15 SWIFT J2058.4+0516 X 20 58 19.898 +05 13 32.25           ~ 169 0
16 ASASSN -15lh ev 22 02 15.4 -61 39 34           ~ 187 1

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