2026A&A...706A.321M


Query : 2026A&A...706A.321M

2026A&A...706A.321M - Astronomy and Astrophysics, volume 706A321 (2026/2-1)

Double-hump spectrum, pulse profile dip, and pulsed fraction spectra from the low-accretion regime in the X-ray pulsar MAXI J0655-013.

MALACARIA C., PIKE S.N., D'AI A., ISRAEL G.L., DUCCI L., ROTHSCHILD R.E., STELLA L., AMATO R., AMBROSI E., COLEY J.B., FURST F., IMBROGNO M., KRETSCHMAR P., MANIADAKIS D.K., PAPITTO A., PRADHAN P., ROUCO ESCORIAL A., SIMONGINI A., STIERHOF J., WEST B.F. and ZALOT N.

Abstract (from CDS):

Context. Accreting X-ray pulsars (XRPs) undergo different physical regimes depending on different mass accretion rates, with related changes in the emitted X-ray spectral properties. Recent observations have shown a dramatic change in the emission properties of this class of sources observed at low luminosity.
Aims. We explore the timing and spectral properties of the XRP MAXI J0655-013 observed in the low-luminosity regime (about 5 × 1033 erg s–1) to witness the corresponding spectral shape and pulse profiles.
Methods. We employed recent XMM-Newton and NuSTAR pointed observations of the MAXI J0655-013 X-ray activity during the low-luminosity stage. We explored several spectral models to fit the data and test theoretical expectations of the dramatic transition of the spectral shape compared to the higher luminosity regime. We studied the pulsating nature of the source and found a precise timing solution. We explored the energy-resolved pulse profiles and the derived energy dependence of different pulsed fraction estimators (PFminmax and PFrms). We also obtained NuSTAR pulsed fraction spectra (PFS) at different luminosity regimes.
Results. The MAXI J0655-013 spectrum is well fit by a double Comptonization model, in agreement with recent observational results and theoretical expectations that explain the observed spectrum as being composed of two distinct bumps, each dominated by different polarization modes. We measured a spin period of 1081.86 ± 0.02 s, consistent with the source spinning up compared to previous observations, yielding an upper limit for the magnetic field strength of B ≲ 9 × 1013 G. The pulse profiles show a single broad peak interrupted by a sharp dip that coincides with an increase in the hardness ratio, and thus likely due to absorption. For the low-luminosity observation, the PFminmax increases with energy up to ∼100% in the 10-30 keV band, while the PFrms remains steady at ∼60%. The PFS obtained at high luminosity shows evidence of an iron Kα emission line but no indications of a cyclotron line.

Abstract Copyright: © The Authors 2026

Journal keyword(s): accretion - accretion disks - polarization

Simbad objects: 12

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Number of rows : 12
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 LIN 198 HXB 00 52 05.6251611744 -72 26 04.228773036 13.86 14.91 14.927 14.91 14.794 B0-5(II)e 187 0
2 SWIFT J0243.6+6124 HXB 02 43 40.4252869512 +61 26 03.757456824   13.71 12.84 12.57   O9.5Ve 208 0
3 V* X Per HXB 03 55 23.0777456088 +31 02 45.039836148 6.090 6.840 6.720     O9.5III 1037 0
4 LS V +44 17 HXB 04 40 59.3296237272 +44 31 49.258049376 11.02 11.42 10.73 10.28 9.76 B0.2Ve 176 0
5 HD 245770 HXB 05 38 54.5748918624 +26 18 56.836952784 9.30 9.84 9.39 8.77 8.30 O9/B0III/Ve 1045 0
6 V* V520 Mon XB* 06 55 12.4349545824 -01 28 53.546183796   12.644 12.498 12.273   O9.5-B0Ve 19 1
7 2MASS J09050682-5330195 XB* 09 05 06.8206433269 -53 30 19.523474160           B1.5-2III-Ve 15 0
8 GRO J1008-571 HXB 10 09 46.9642314696 -58 17 35.603851848       14.63   B0e 269 0
9 V* V850 Cen HXB 13 01 17.0968941216 -61 36 06.637549788   15.6 14.40     B2Vne 361 0
10 IGR J13020-6359 HXB 13 01 58.7205396744 -63 58 08.828687136           B0.5Ve 68 0
11 4U 1416-62 HXB 14 21 12.1560262026 -62 41 56.089360085   17.9 17.2     B1e 171 0
12 V* V2246 Cyg HXB 20 32 15.2749858128 +37 38 14.843024844   22.16 19.41 17.32 15.18 B0Ve 480 0

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