2025ApJ...988..153R


Query : 2025ApJ...988..153R

2025ApJ...988..153R - Astrophys. J., 988, 153 (2025/August-1)

A Multi-wavelength Characterization of the 2023 Outburst of MAXI J1807+132: Manifestations of Disk Instability and Jet Emission.

ROUT S.K., BAGLIO M.C., HUGHES A.K., RUSSELL D.M., BRAMICH D.M., SAIKIA P., ALABARTA K., ARMAS PADILLA M., CAMPANA S., COVINO S., D'AVANZO P., FENDER R., GOLDONI P., HOMAN J., LEWIS F., MASETTI N., MOTTA S., MUNOZ-DARIAS T., PAPITTO A., RUSSELL T.D., SIVAKOFF G. and VAN DEN EIJNDEN J.

Abstract (from CDS):

Several phenomenological aspects of low-luminosity neutron star transients, such as atolls, remain poorly understood. One such source, MAXI J1807+132, entered its latest outburst in 2023 July. To thoroughly characterize this outburst, we conducted an extensive observational campaign spanning radio to X-ray wavelengths. Here we present the results of this campaign, which covered the period from before the outburst to the return to quiescence. We detected a delay between the X-ray and optical rise times, which is consistent with the predictions of the disk instability model with a truncated disk. The color evolution and optical/X-ray correlations, along with infrared and radio detections, support the presence of jet synchrotron emission during the gradual decay phase following the peak. We also report for the first time in an X-ray binary a near-orthogonal rotation of the optical polarization just before a small flare, after which the jet is thought to be quenched. The main outburst is followed by several high-amplitude, rapid reflares in the optical, ultraviolet, and X-ray bands, the origin of which remains difficult to constrain.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Low-mass x-ray binary stars - Neutron stars - Jets - Accretion

Simbad objects: 18

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Number of rows : 18
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 V* V1037 Cas LXB 00 29 03.06 +59 34 19.0           ~ 283 1
2 X LMC X-3 HXB 05 38 56.6323605504 -64 05 03.317937504   17 17.2     B2.5Ve 722 0
3 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
4 V* V822 Cen LXB 14 58 21.9347842080 -31 40 07.515432768 11.95 12.85 12.8     K3-K7V 555 0
5 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
6 [KRL2007b] 214 LXB 17 00 58.46 -46 11 08.6           ~ 296 0
7 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
8 MAXI J1807+132 LX? 18 08 07.549 +13 15 05.40           ~ 53 0
9 SAX J1808.4-3658 LXB 18 08 27.58 -36 58 43.9           ~ 1051 0
10 V* NP Ser LXB 18 16 01.7 -14 02 09   18.8       K 683 2
11 X Sgr X-4 LXB 18 23 40.57 -30 21 40.6   19.06 18.81     ~ 1056 1
12 V* MM Ser LXB 18 39 57.8 +05 02 13   19.2 19.2     ~ 378 0
13 BD-12 5133 * 18 40 01.6961497488 -12 24 06.777653508 11.25 11.39 10.71 10.70   OB- 44 0
14 SWIFT J1858.6-0814 XB* 18 58 34.91 -08 14 14.8           ~ 76 0
15 MAXI J1910-057 LXB 19 10 22.80 -05 47 55.9           ~ 84 0
16 X Aql X-1 LXB 19 11 16.0571313336 +00 35 05.868232692           ~ 1186 1
17 V* V1408 Aql LXB 19 59 24.0074252040 +11 42 29.859773292 18.40 18.97 18.95 18.70 18.66 ~ 234 0
18 V* V404 Cyg HXB 20 24 03.8247037434 +33 52 01.961154861           G9/K0III/V 1370 0

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