The mHz quasi-regular modulations of 4U 1630−47 during its 1998 outburst

Author:

Zhao Q C123ORCID,Yin H X1,Tao L2,Yang Z X23,Qu J L2,Zhang L2ORCID,Zhang S2,Qiao E L45,Bu Q C6ORCID,Zhao S J23,Li P P23,Huang Y M23,Ma R C23ORCID,Tang R J7,Jin P23,Yu W23,Liu H X23,Huang Y2,Ma X2,Xiao J Y23,Zhang X2,Zhao K23

Affiliation:

1. Shandong Key Laboratory of Optical Astronomy and Solar-Terrestrial Environment, School of Space Science and Physics, Institute of Space Sciences, Shandong University , Weihai, Shandong 264209, China

2. Key Laboratory of Particle Astrophysics, Institute of High Energy Physics, Chinese Academy of Sciences , Beijing 100049, China

3. University of Chinese Academy of Sciences, Chinese Academy of Sciences , Beijing 100049, China

4. Key Laboratory of Space Astronomy and Technology, National Astronomical Observatories, Chinese Academy of Sciences , Beijing 100101, China

5. School of Astronomy and Space Sciences, University of Chinese Academy of Sciences , 19A Yuquan Road, Beijing 100049, China

6. Institut für Astronomie und Astrophysik, Kepler Center for Astro and Particle Physics, Eberhard Karls Universität , Sand 1, D-72076 Tübingen, Germany

7. Beijing Jiaotong University , Beijing 100044, China

Abstract

ABSTRACT We present the results of a detailed timing and spectral analysis of the quasi-regular modulation (QRM) phenomenon in the black hole X-ray binary 4U 1630−47 during its 1998 outburst observed by the Rossi X-ray Timing Explorer (RXTE). We find that the ∼50–110 mHz QRM is flux dependent, and the QRM is detected with simultaneous low-frequency quasi-periodic oscillations (LFQPOs). According to the behaviour of the power density spectrum, we divide the observations into four groups. In the first group, namely behaviour A, LFQPOs are detected, but no mHz QRM. The second group, namely behaviour B, a QRM with frequency above ∼88 mHz is detected and the ∼5 and ∼7 Hz LFQPOs are almost overlapping. In the third group, namely behaviour C, the QRM frequency below ∼88 mHz is detected and the LFQPOs are significantly separated. In the fourth group, namely behaviour D, neither QRM nor LFQPOs are detected. We study the energy dependence of the fractional rms, centroid frequency, and phase lag of QRM and LFQPOs for behaviour B and C. We then study the evolution of QRM and find that the frequency of QRM increases with hardness, while its rms decreases with hardness. We also analyse the spectra of each observation, and find that the QRM rms of behaviour B has a positive correlation with $F_{\rm power\ law}$/$F_{\rm total}$. Finally, we give our understanding for this mHz QRM phenomenon.

Funder

Natural Science Foundation of China

National Natural Science Foundation of China

CAS

NAOC

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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