2023A&A...680A..88S


Query : 2023A&A...680A..88S

2023A&A...680A..88S - Astronomy and Astrophysics, volume 680A88 (2023/12-1)

NuSTAR and XMM-Newton observations of the binary 4FGL J1405.1-6119 A γ-ray-emitting microquasar?

SAAVEDRA E.A., FOGANTINI F.A., ESCOBAR G.J., ROMERO G.E., COMBI J.A. and MARCEL E.

Abstract (from CDS):

Context. 4FGL J1405.1-6119 is a high-mass γ-ray-emitting binary that has been studied at several wavelengths. The nature of this type of binary is still under debate, with three possible scenarios usually invoked to explain the origin of the γ-ray emission: collisions between the winds of a rapidly rotating neutron star and its companion, collisions between the winds of two massive stars, and nonthermal emission from the jet of a microquasar.
Aims. We analyzed two pairs of simultaneous NuSTAR and XMM-Newton observations to investigate the origin of the radio, X-ray, and γ-ray emissions.
Methods. We extracted light curves between 0.5 and 78 keV from two different epochs, which we call Epoch 1 and Epoch 2. We then extracted and analyzed the associated spectra to gain insight into the characteristics of the emission in each epoch. To explain these observations, along with the overall spectral energy distribution, we developed a model of a microquasar jet. This allowed us to make some inferences about the origin of the observed emission and to discuss the nature of the system.
Results. A power-law model combined with the inclusion of a blackbody accurately characterizes the X-ray spectrum. The power-law index (E–Γ) was found to be ∼1.7 for Epoch 1 and ∼1.4 for Epoch 2. Furthermore, the associated blackbody temperature was ∼1 keV and with a modeled emitting region of size ≲16 km. The scenario we propose to explain the observations involves a parabolic, mildly relativistic, lepto-hadronic jet. This jet has a compact acceleration region that injects a hard spectrum of relativistic particles. The dominant nonthermal emission processes include synchrotron radiation of electrons, inverse Compton scattering of photons from the stellar radiation field, and the decay of neutral pions resulting from inelastic proton-proton collisions within the bulk matter of the jet. These estimates are in accordance with the values of a super-Eddington lepto-hadronic jet scenario. The compact object could be either a black hole or a neutron star with a weak magnetic field. Most of the X-ray emission from the disk could be absorbed by the dense wind that is ejected from the same disk.
Conclusions. We conclude that the binary 4FGL J1405.1-6119 could be a supercritical microquasar similar to SS 433.

Abstract Copyright: © The Authors 2023

Journal keyword(s): X-rays: binaries - gamma rays: stars

Simbad objects: 15

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Number of rows : 15
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 LS I +61 303 HXB 02 40 31.6644419688 +61 13 45.593918580 11.27 11.61 10.75 10.19 9.55 B0Ve 903 2
2 4FGL J0535.2-6736 HXB 05 36 00.01 -67 35 07.5           ~ 49 0
3 HD 259440 HXB 06 32 59.2566076656 +05 48 01.160755848 9.17 9.63 9.15     B0pe 256 0
4 * gam02 Vel WR* 08 09 31.95013 -47 20 11.7108 0.64 1.58 1.83 1.85 2.00 WC8+O7.5III-V 951 0
5 1FGL J1018.6-5856 HXB 10 18 55.5875706288 -58 56 45.975246900   13.638 12.683     O6V((f)) 156 0
6 * eta Car s*b 10 45 03.545808 -59 41 03.95124 6.37 7.03 6.48 6.123 4.41 LBV 2543 0
7 CPD-63 2495 HXB 13 02 47.6544015048 -63 50 08.626970292 10.34 10.72 9.98 10.03   O9.5Ve 852 0
8 2MASS J14051441-6118282 HXB 14 05 14.41560 -61 18 28.2168           O6.5III 53 0
9 AX J1600.9-5142 WR* 16 00 50.47872 -51 42 44.9784           WC8+WN4-6b 27 1
10 V* V479 Sct HXB 18 26 15.0561548880 -14 50 54.247274304 12.02 12.23 11.27 11.04   ON6V((f))z 613 2
11 2MASS J18324516-0921545 XB* 18 32 45.162 -09 21 54.55           ~ 37 0
12 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A7Ib 2253 4
13 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
14 [MT91] 213 Psr 20 32 13.1247390384 +41 27 24.346666440 13.12 13.08 11.266     B0Vp 334 0
15 V* V1521 Cyg HXB 20 32 25.78 +40 57 27.9           WN4/5-6/7 2035 2

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