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2021ApJ...913..119J - Astrophys. J., 913, 119-119 (2021/June-1)

Study on the energy limits of kHz QPOs in Sco X-1 with RXTE and Insight-HXMT observations.

JIA S.M., QU J.L., LU F.J., ZHANG S.N., ZHANG S., HUANG Y., WANG D.H., ZHOU D.K., XIAO G.C., BU Q.C., CHEN L., MA X., SONG L.M., TAO L., CAO X.L., CHEN Y., LIU C.Z. and XU Y.P.

Abstract (from CDS):

We present a detailed spectral-timing analysis of the Kilohertz quasiperiodic oscillations (kHz QPOs) in Sco X-1 using the data of the Rossi X-ray Timing Explorer (RXTE) and the Hard X-ray Modulation Telescope (Insight-HXMT). The energy band with detectable kHz QPOs is studied for the first time: on the horizontal branch, it is ∼6.89-24.01 and ∼8.68-21.78 keV for the upper and lower kHz QPOs, respectively, detected by the RXTE, and ∼9-27.5 keV for the upper kHz QPOs by the Insight-HXMT; on the lower normal branch, the energy band is narrower. The fractional root mean square (rms) of the kHz QPOs increases with energy at a lower energy, reaches a plateau at about 16 and 20 keV for the lower and upper peaks, and then levels off though with a large uncertainty. The simulation of the deadtime effect of RXTE/PCA shows that the deadtime does not affect much the search of the kHz QPOs but makes the rms amplitude underestimated. No significant QPO is detected below ∼6 keV as shown by the RXTE data, implying that the kHz QPOs do not originate from the blackbody emission of the accretion disk and neutron star surface. In addition, with the combined analysis of the energy spectra and the absolute rms spectra of kHz QPOs, we suggest that the kHz QPOs in Sco X-1 originate from the Comptonization of the inner part of the transition layer, where the rotation sets the frequency and the inward bulk motion makes the spectrum harder.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): X-ray binary stars

Simbad objects: 7

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