基于Jurkevich法Cyg X-1光变周期特性研究

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Cyg X-1近16年的Rossi X-ray Timing Explorer(RXTE)All-Sky Monitor(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Cyg X-1存在363±11.5 d的光变周期,但没有发现420 d的光变周期,而且150 d的光变周期可能仅仅是51±1.4 d光变周期的观测表象。     

用Jurkevich方法分析计算BL Lac天体的光变周期

本文介绍一种分析寻找ＢＬＬａｃ天体光变周期的方法,给出了ＢＬＬａｃ天体ＯＪ２８７,ＯＮ２３１,Ｍｒｋ４２１的长光变周期．分析计算表明：当观测样品的数据点很多、观测时间很长（大约１００年左右的光学波段数据）、数据样本不少于６个周期并能从光变曲线的两次大振幅中,看出有若干小振幅的周期时,则能用该方法准确地认证和确定其长周期值．这种方法在寻找周期时,对无规律不等间隔的样品数据有较高的灵敏度,而计算方法简捷实用,结果可靠     

CygX-1 X辐射的功率谱

运用自回归功率谱研究CygX－1X辐射的频谱特征,结果显示CygX－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加噪声成分描述,转换态存在小于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谱描述,不存在显著的QPO．截断频率在各态都相当稳定,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,自回归功率港分析是研究X射线双星光变特征的一个有效的方法．     

类星体3C345的光变周期特性研究

从大量文献资料中,收集了类星体3C345光学B波段的有效观测数据点共1642个,获得了从1896年至1993年的历史光变曲线．用Jurkevich方法计算分析3C345的光变周期,结果表明3C345的长光变周期为10．1±0．8年（或21．8±1．5年）,预期2002年1月应该为再次爆发期．     

判定光变周期的一种方法

Jurkevich方法通常用来发现光变曲线的周期，并且根据Vm^2极小值的大小来验证所发现的光变周期可靠性。但是，这种验证方法又带有一定的不确定性，最佳的方法是把所发现的周期与观测光变曲线拟合，得出每一个周期的振幅，以振幅大小来验证所发现的光变周期的可靠性。将此方法用于OJ287的历史光变曲线，得到其最主要的周期为11．9年，与其它结果相符合。     

判定光变周期的一种方法

Jurkevich方法通常用来发现光变曲线的周期 ,并且根据V2 m 极小值的大小来验证所发现的光变周期可靠性。但是 ,这种验证方法又带有一定的不确定性 ,最佳的方法是把所发现的周期与观测光变曲线拟合 ,得出每一个周期的振幅 ,以振幅大小来验证所发现的光变周期的可靠性。将此方法用于OJ2 87的历史光变曲线 ,得到其最主要的周期为 11.9年 ,与其它结果相符合。     

BLLac天体ON231的光变周期研究

从大量文献中收集了BLLac天体ON231光学B波段约100年的观测数据,在此基础上分析了光变周期。用两种不同的方法（Jurkevich方法和小波分析法）分析周期光变,发现其光变曲线中存在13．6±1．5及26．1年的周期。     

类星体3C273的多波段光变周期分析

从文献中收集了类星体3C273射电、毫米、红外、光学、紫外和高能波段1963年至2006年的观测数据,获得各波段的长期光变曲线。用Jurkevich方法和离散相关函数(Discrete Correlation Function,DCF)方法分别研究了多波段的光变周期。研究结果表明:(1)3C273在所研究波段内的辐射流量都表现出周期性变化的特征;(2)用Jurkevich方法和离散相关函数方法分析得到的多波段变化周期的结果非常一致;(3)3C273在射电和毫米波段可能存在8.0年左右的固有周期成分,在红外、光学和紫外波段可能存在2.0年和11.0年左右的固有周期成分,在高能波段可能存在1.0年左右的固有周期成分。简要探讨了引起3C273各波段周期光变的可能原因,研究结果表明用激波加速模型(shock-in-jet)能较好地解释引起3C273多波段光变的原因。     

基于最大熵谱估计的高能电子周期特性研究

利用最大熵谱法研究了风云二号D星≥2.0 MeV的高能电子通量的周期特性,算法以自相关模型为基础,通过对最大熵谱功率谱的分析,推测出风云二号D星高能电子通量存在13.87 d和27.8 d的周期.根据最终预报误差准则(Final Prediction Error,FPE)和赤池信息量准则(Akaike Informat...     

黑洞候选体X射线双星Cyg X-1硬度比周期特性研究

利用离散傅里叶分析法,基于RXTE (Rossi X-ray Timing Explorer)/ASM(All-Sky Monitor,1.5～12 keV)观测数据,对黑洞候选体X射线双星Cyg X-1硬度比HR(5～12 keV/3～5 keV)(简写HR)的时变特性进行了分析,结果表明黑洞候选体X射线双星Cyg X-1硬度比HR存在明显的周期特性:(1)混合态(硬态+软态,本文指MJD=50087～55841期间所有的观测数据)时,HR存在T≈5.6 d、40.0 d、78.4 d、173.8 d以及400/800 d的时变周期; (2)硬态时, HR存在T≈5.6 d、33.7/67.6 d、45.3 d和165.3 d的周期特性; (3)软态时,HR出现了T≈38.5 d、48.1 d和128.3 d的周期性变化.并利用粘滞理论和Zdziarski吸积盘模型讨论了以上周期特性的物理机制.     

A Study on the Long-term Spectral Variability of the Black-hole Candidate X-ray Binary Cyg X-1

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.     

Results of Light Curve Analysis of the Massive Binary Cyg X-1/V1357 Cyg in Primary Minimum

The results of new UBV photometric observations of V1357 Cyg in primary minimum are presented. Observations were carried out from 1996 up to now with 60 cm telescope in Crimea with the goal to study additional radiation that was detected in the mean light curve of this system near orbital phase 0.0. The properties of this additional radiation are also considered.     

The additional radiation of Cyg X-1 at primary minimum

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).     

A Study on the Periodicity of Hardness Ratio of the X-ray Binary Cyg X-1 as a Black Hole Candidate

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.     

黑洞候选体X射线双星Cyg X-1光变曲线的研究

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．     

The short timescale bursts of Cyg X-1 in the high and transitional states

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.     

The time lag of high-energy photons of Cyg X-1 in hard state

The time lag between hard and soft X-rays is an important aspect of the study of high-energy emission. Fourier cross spectrum, often used in calculating the time lag, is unable to measure statistically significant fast light variation above Fourier frequency 30 Hz from the measurements of Cyg X-1. The method of cross correlation function in time domain, developed by Li Ti-pei, can be effectively used in measuring time lags on different time scales. Using Li's method we discuss the properties of the time lag of high-energy photons of Cyg X-1 in hard state at different times. The results show that there is a significant time lap on short times scales (< 0.1 s). We confront different models of hard-state Cygnus X-1 with the observed time lag.     

Cyg X-1高态中短暴性质的研究

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．