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1.
运用自回归功率普研究Cyg X-1 X辐射的频谱特征,结果显示Cyg X-1转换态和高/软态时变频谱的连续成分,可以统一由有截断的幂律的成分描述,转换态存在小地3HZ的宽峰结构及准周期振荡(QPO)成分(4-12HZ),而高/软态完全可由截断幂律普描述,不存在显著的QPO。截断频率在各态相相当,在不同态的演化与平流为主的吸积流模型(ADAF(预期的情形一致。本文结果表明,自回归功率 研究X射线双 相似文献
2.
针对天文观测数据不等间隔的特点,利用Jurkevich方法对黑洞候选体x射线双星CygX-1近16年的RossiX-rayTimingExplorer(RXTE)All-SkyMonitor(ASM)数据进行了频谱分析,并结合Kidger周期存在可信度的判据,发现CygX-1存在363±11.5d的光变周期,但没有发现420d的光变周期,而且150d的光变周期可能仅仅是51±1.4d光变周期的观测表象。 相似文献
3.
分析RXTE卫星PCA探测器对CygX-1的观测数据,得到了其处于高态及高低态转换时的X射线短时标爆发(Shot)结构.在所观测到的三种态中是不对称的,并且不同的状态中Shot的结构有明显差异.Shot前后沿可分别由双指数函数近似拟合.Shot中的快时变过程是由慢的上升前沿和快的下降后沿构成.在所观测态中Shot平均宽度约为0.11秒(FWHM),比低态时的宽度窄.同一状态中高能段的Shot宽度较低能段窄,且更加不对称.转换态的硬度在Shot峰前有明显下降,之后迅速上升,Shot期间的平均硬度低于非Shot期平均值;而高态时峰前硬度没有明显下降,Shot期间的平均硬度高于非Shot期间的平均值.本文还就Shot的产生机制进行了讨论. 相似文献
4.
能谱仅反映了高能天体辐射的部分性质,而高能X射线辐射的时变可以反映致密天体的动态性质。因此,在构造高能辐射的理论模型时,既要考虑X辐射的能谱性质,也要考虑其时变性质。特别对高能天体X辐射的快速光变,一般认为其发生在致密天体附近,致密天体快速光变的研究可以揭示出致密天体附近的物理性质,因此,时变可以对X辐射模型给以很强的限制。X射线源不同能量光子到达观测者的时间差称为X射线辐射的时延。介绍了高能X辐射时变中的时延分析方法及其最新发展,综述了致密双星系统中黑洞侯选林和中子星的时延现象,并简单介绍了为解释这些现象所发展的模型,以及时延对模型的限制。 相似文献
5.
采用含有频率涨落噪声和指数形式关联随机力作用的广义朗之万(Langevin)方程模型描述黑洞吸积盘的垂向振荡,推导出吸积盘随机振荡光度功率谱密度的解析表达式,并讨论了系统参数对功率谱密度中低频准周期振荡(Low Frequency Quasi-Periodic Oscillations,LFQPOs)现象的影响。研究结果发现选取合适的系统参数时,功率谱密度曲线上出现了一个基频和一个二次谐频的共振双峰低频准周期振荡,基频峰对应的中心频率为吸积盘振荡的特征频率;随机力关联时间决定了基频峰的高度和宽度,频率噪声强度和粘滞阻尼只对二次谐频峰产生影响。结果说明吸积盘的随机振荡模型可以作为低频准周期振荡起源的一种解释。 相似文献
6.
分析RXTE卫星PCA探测器对CygX-1的观测数据,得到了其处于高态及高低高转换时的X射线短时标爆发(Shot)结构。在所观测到的三种态中是不对称的,并且不同的状态中Shot的结构有明显差异。Shot前后沿可分别由双指数函数近似拟合。Shot中的快时变过程是由慢的上升前沿和快的下降后沿构成。在所观测态中Shot平均宽度约为0.11秒(FWHM),比低态时的宽度窄。同一状态中高能段的Shot宽度较 相似文献
7.
通过分析1997年2月27日和3月1日坚天座座X-1的两次空间数据观测。发现千赫兹QPO频率同X射线能谱有一定相关,其和赤类似于另一个X射线同源4U1605-52,讨论了分析结果对了解吸积及QPO产生过程的意义。 相似文献
8.
利用Rossi X-ray Timing Explorer(RXTE)卫星从1996年1月5日到2005年5月1日的all-sky monitor(ASM,1.5-12KeV)资料,详细分析了黑洞候选体X射线双星Cyg X-1在A-band(1.5-3KeV),B-band(3-5KeV)和C-band(5-12KeV)三个能段上光子计数率与谱线硬度比HR2(5-12KeV/3-5KeV)的相关性.利用1天时标的ASM资料研究发现: (1)Cyg X-1处于软态时,在A-band上光子计数率与硬度比HR2呈现反相关性,而在B-band和C-band上呈现正相关性.当该天体处于硬态时,在A、B、C三个能段上光子计数率与硬度比HR2都是反相关的.(2)Cyg X-1处于硬态和软态时,硬度比HR2与HR1都是正相关的.此外,还分析了ASM上"Dwell by Dwell"资料,得到了十分有趣的结果,即: (1)MJD=52600-52760期间(此时Cyg X-1处于硬态),A-band和B-band上的光子计数率与HR2是反相关性的,而在C-band上却呈现出较强的正相关性. (2)硬态时,硬度比HR2与HR1存在明显的反相关性. 相似文献
9.
通过分析1997年2月27日和3月1日对天鹰座X-1的两次空间数据观测.发现千赫兹QPO频率同X射线能诺有一定相关,其行为类似于另一个X射线暂现源4U1608-52,讨论了分析结果对了解吸积及QPO产生过程的意义. 相似文献
10.
本文采用了多方物态方程p=kρ^(1+1/n)研究了在黑洞附近跨声速α吸积盘的径向线性稳定性,在导出扰动色散关系时考虑了吸积流的径向运动速度,结果表明粘滞系数α存在一上限αc,当α>αc时,吸积流是不稳定的,αc与多方指数n及吸积流的径向速度vr有关。 相似文献
11.
Short timescale bursts or “shots” of Cyg X-1 in one ms time bins were obtained from PCA/RXTE observation. By superposing many shots lined up at the peak, a mean profile was obtained, and this was done seperately for the different states, high, transitional and low. The mean shot profile is different for the different states. The duration of shot is shorter in the high than in the transitional state. In both, the duration is about 0.11 s, which is shorter than in the low state. The profile is more asymmetrical in high than in low energy bands. In the transitional state, the average hardness during shots is lower than that of the steady component. The mechanism of shot generation is discussed. 相似文献
12.
Using the All-Sky Monitor (ASM, 1.5–12–kev) data of Rossi X-ray Timing Explorer (RXTE) from January 1996 to May 2005, we have made a detailed analysis of the correlation between photon-count rate and spectral hardness ratio HR2 (5–12 keV/3–5 keV) of the black-hole candidate X-ray binary Cyg X-1 in 3 energy bands, namely the A-band (1.5–3 keV), B-band (3–5 keV) and Cband (5–12 keV). By the study on the ASM data of 1-day time scale, we find: (1) When Cyg X-1 is in the soft state, the A-band photon-count rate and hardness ratio HR2 exhibit an anticorrelation, but in B-band and C-band there appears the positive correlation. When Cyg X-1 is in hard state, the photon-count rates in the A,B,C bands are all inversely correlated with the hardness ratio HR2; (2) No matter whether Cyg X-1 is in the soft state or the hard state, the hardness ratios HR2 and HR1 are always positively correlated. In addition, we have analyzed the “dwell by dwell” data of the ASM, and obtained the following interesting results: (1) In the period of MJD = 52600–52760 (while Cyg X-1 is in the hard state), the photon-count rates in the A-band and B-band are inversely correlated with HR2, but in the C-band there appears a relatively strong positive correlation; (2) During the hard state, a clear anticorrelation exists between the hardness ratios HR2 and HR1. 相似文献
13.
利用Rossi X-ray Timing Explorer(RXTE)卫星从1996年1月到2005年5月的公共资料,研究了黑洞候选体X射线双星Cyg X-1光变曲线的周期性,并且发现了一些有趣的周期特性(T=1.0±0.2天和T=18.0±3.0天).在硬态时,T=1.0±0.2天和T=18.0±3.0天的周期特性同时出现在它的光变曲线之中,但在软态时仅有T=1.0±0.2天的周期出现.采用一种新的方法(即微分法),同时为了检验微分法的正确性,还利用传统的方法(即快速傅立叶变换和叠加法)分析了相同的资料,并得到了与微分法相同的结果.另外也对Cyg X-1的轨道周期进行了研究,结果发现T=5.6天的轨道周期不仅出现在硬态,同时也出现在软态,只是在硬态时比在软态时明显. 相似文献
14.
CygX-1高能辐射的时变特征可以通过短暴(shot)的性质反映.因此CygX-1的短暴性质,特别是处于低态时的性质曾被广泛研究,利用直接叠加短暴和自相关函数,对CygX-1高态时短暴的性质进行了研究.结果表明,当CygX-1处于高态时,其短暴的结构类似于低态时所具有的性质,短暴的半高宽随能量的增加按指数下降.此结果和康普顿化模型不一致.另外,短暴的能谱演化及结构的非对称性可以解释CygX-1中的时延现象. 相似文献
15.
New UBV-photoelectric observations of the well-known massive X-ray binary system Cyg X-1/V 1357 Cyg are obtained near the primary minimum. The detailed analysis of these observations confirms the existence of additional blue radiation which appears as a narrow peak with an amplitude of 0.01–0.02 mag near phase 0.00 on the light curve (the superior conjunction of the relativistic component), firstly detected by Lyuty (1985). This emission does not appear at every orbital cycle. The appearance of this narrow peak of additional blue radiation on the light curve of Cyg X-1 can be explained as the radiation of relativistic electrons in the disturbed magnetic field of the optical star in frames of the model proposed by Ikhsanov and Fabrika (1990). 相似文献
16.
R. K. Manchanda 《Journal of Astrophysics and Astronomy》2001,22(1):9-20
The black hole candidate Cyg X-1 was observed in ultra low state on march 30, 1997 using Large Area Scintillation counter
Experiment (LASE) in the hard X-ray energy region of 20–180 keV. During the 30 minute exposure a combined signal of 68 sigma
was obtained, however, the measured flux at 50 keV was lower by a factor of 2 than the minimum flux reported so far. Using
the recent orbital ephemeris of the source, our snap-shot observations were made at ϕ5.6 = 0.915, which corresponds to the binary minimum revealed by the ASM light curves. The daily average data from the BATSE
detectors give the source intensity level to be higher by a factor of 5. Very low flux values measured in the present experiment
suggest that the hard X-ray source may have been partially occulted by the primary companion during its transit near the X-ray
minimum. 相似文献
17.
18.
Using the All-Sky Monitor (ASM, 1.5∼12 keV) data of Rossi X-ray Timing Explorer (RXTE) from January 1996 to October 2011, we have analyzed in detail the power spectrum of the hardness ratio (HR) (5∼12 keV/3∼5 keV) of the X-ray binary Cyg X-1 as a black hole candidate. The results show that the HR exhibits the following periodical variations: (1) During MJD = 50087∼55841, the HR presented the the periods T ≈ 5.6 d, T ≈ 40.0 d, T ≈ 78.4 d, T ≈ 173.8 d, and T ≈ 400/800 d; (2) When Cyg X-1 was in the hard state, the HR exhibited the periods T ≈ 5.6 d, T ≈ 33.7/67.6 d, T ≈ 45.3 d, and T ≈ 165.3 d; (3) When Cyg X-1 was in the soft state, the HR exhibited the periods T ≈ 38.5 d, T ≈ d, and T ≈ 128.3 d. Moreover, using the viscosity theory and Zdziarski accretion disk model, we have made a discussion on the physical mechanism of this kind of periodicity. 相似文献
19.
M. Gilfanov E. Churazov M. Revnivtsev 《Monthly notices of the Royal Astronomical Society》2000,316(4):923-928
Using RXTE /PCA data, we study the fast variability of the reflected emission in the soft spectral state of Cyg X-1 by means of Fourier frequency-resolved spectroscopy. We find that the rms amplitude of variations of the reflected emission has the same frequency dependence as the primary radiation down to time-scales of ≲30–50 ms. This might indicate that the reflected flux reproduces, with nearly flat response, variations of the primary emission. Such behaviour differs notably from that of the hard spectral state, in which variations of the reflected flux are significantly suppressed in comparison with the primary emission, on time-scales shorter than ∼0.5–1 s.
If related to the finite light-crossing time of the reflector, these results suggest that the characteristic size of the reflector, presumably an optically thick accretion disc, in the hard spectral state is larger by a factor of ≳5–10 than in the soft spectral state. Modelling the transfer function of the disc, we estimate the inner radius of the accretion disc to be Rin ∼100 R g in the hard state and R in ≲10 R g in the soft state for a 10-M⊙ black hole. 相似文献
If related to the finite light-crossing time of the reflector, these results suggest that the characteristic size of the reflector, presumably an optically thick accretion disc, in the hard spectral state is larger by a factor of ≳5–10 than in the soft spectral state. Modelling the transfer function of the disc, we estimate the inner radius of the accretion disc to be R