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．     

基于Jurkevich法CygX-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。     

BL Lac天体ON 231的光变周期研究

从大量文献中收集了BL Lac天体ON 231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。     

AO0235＋164射电波段宽带谱指数周期性变化的研究

收集了AO0235＋164天体射电4．8GHz和14．5GHz波段的光变测量数据,并获得了长期的光变曲线,从光变曲线可以看出其活动是非常剧烈的。利用Jurkevieh方法和自相关函数方法分别对AO0235＋164射电波段宽带谱指数进行周期性分析,并对流量和谱指数进行相关性分析,研究结果表明：（1）AO0235＋164天体射电波段4．8GHz-14．5GHz对应的宽带谱指数,可能存在5．30年的光变周期,与Liu等人用功率谱法在射电波段发现其流量密度可能存在5．59±0．47年的光变周期基本吻合;（2）宽带谱指数与流量密度之间存在相关性。     

基于自回归方法的Blazar天体3C 279和OJ 287光变周期研究

探索Blazar光变资料中的周期或准周期变化是1个有待深入研究的领域.由于光变资料的复杂性,目前寻找周期的算法还不够完善.文中以现代谱估计为基础,详细论述了自回归(Auto-regressive,AR)模型谱估计方法和最大熵谱估计的基本原理,分析了阶数选择对模型的重要影响,并把这些方法应用到类星体3C 279和BL Lac天体OJ287的光变周期分析中,得到它们的光变周期分别为7.14和11.76yr.通过验证,自回归 模型谱估计方法由于其分辨率高,可以作为1种较好的分析周期的方法.最后指出在应用谱估计分析Blazar天体的光变周期注意事项.     

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     

类星体长周期光变分析方法的研究

给出了4种分析类星体长周期光变的方法,用一个模拟的周期信号y=sinθ检验这4种分析方法,结果表明:(1)天体光变采样的数据点个数相对少到一定值时,Jurkevich方法、时间补偿离散傅里叶变换分析方法(DCDFT)、离散相关分析方法(DCF)和功率谱密度分析方法(PSD)的分析结果不一样,获取最短的连续数据点后,Jurkevich方法分析结果在4种方法中可能最为精确可靠,且计算方法简捷实用;(2)获得了Jurkevich分析方法的最佳参数,当m=9时分析结果最佳;(3)用m=9时的Jurkevich方法分析了类星体3C 279及3C 454.3的光变周期,得出3C 279的可能光变周期为(2.81±0.54)年,3C 454.3的可能光变周期为457 d。     

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。     

Blazars天体的多波段的理论研究

在收集大量资料的基础上,较为全面的综述了Ｂｌａｚａｒｓ天体的基本观测特征,给出了目前较为完整的ＢＬＬａｃ天体总表。对该类天体的相关理论,多波段相关性,光变周期分析,Ｈｕｂｂｌｅ关系,ＢＬＬａｃ天体的偏振度的变化作了一定研究。并介绍了我们用ＣＣＤ测光和光谱对３Ｃ３４５作准同时性观测的结果,我们讨论了３Ｃ３４５的历史光变曲线和光变周期分析,研究结果表明：３Ｃ３４５具有（１０±０．８）ａ（年）的光变周期,其中心有一个１０６Ｍ⊙的黑洞。Ｊｕｒｋｅｖｉｃｈ方法是一种Ｂｌａｚａｒｓ天体的光变周期分析研究的好方法     

Period of Light Variability in BL Lac ON 231

In this paper, the authors have compiled the data of about 100 years in B-band of the BL Lac ON 231 and used this database to analyze periodicity signals in the optical light curve. Two different methods were applied: the wavelet analysis and the Discrete Correlation Function (DCF) method. We revealed the existence of periods of 13.5 years in the source variability.     

Discovery of a cyclic period change in the contact binary system V1128 Tau

We obtained several epochs of light minima and a complete R light curve of the W-type contact binary V1128 Tau in 2009. Two cool spots on the massive component are used to model the photometric light curve. Using all available data we find evidence for a long-term period variation with an amplitude of 0.0050±0.0012 days and a period of 16.7±0.9 years. Using parameters derived from a photometric model of the 2009 light curve we show that this period change could be explained by the Applegate mechanism on one of the components.     

Analysis of the V light curve of the system CW Cas

The V light curve of CW Cas, observed during 1972, has been analysed by different methods of solution. The results show great differences between rectifiable and direct methods.     

Blazar天体3C 66A光学波段准周期光变分析

研究了Blazar天体3C 66A光学波段的准周期光变行为.收集了3C 66A光学V波段将近18 yr (2003—2021年)的测光数据,观测数据主要来源是:上海天文台(ShAO)、 AAVSO (The American Association of Variable Star Observers)数据库、Steward天文台.使用了Jurkevich和Lomb-Scargle两种方法分析了光变数据.Jurkevich方法得到了(850±90) d (～2.3 yr)和(1150±140) d (～3.2 yr)的光变周期,而Lomb-Scargle方法在充分考虑了“红噪声”效应之后同样得到了(869±70) d和(1111±90) d的光变周期,它们的置信水平分别为>99%和> 95%.通过与之前的研究结果比较,发现～2.3 yr的光变周期在3C 66A的历史光变数据中是一个稳定的周期,而～3.2 yr的周期则是不稳定的.     

On the apsidal motion of BP Vulpeculae

BP Vulpeculae is a bright eclipsing binary system showing apsidal motion. It was found in an earlier study that it shows retrograde apsidal motion which contradicts theory. In this paper we present the first BV light curve of the system and its light curve solution as well as seven new times of the minima from the years 1959–1963. This way we could expanded the baseline of the investigation to five decades. Based on this longer baseline we concluded that the apsidal motion is prograde agreeing with the theoretical expectations and its period is about 365 years and the determined internal structure constant is close to the theoretically expected one.     

3C273的光学光变周期

收录了类星体3C273约110年的光学资料，并在此基础上讨论了光变周期性.当用两种不同方法(Jurkevich方法及DCF(离散相关系数)法)分析时，发现光变曲线中存在周期为2.0年、(13.65±0.20)及(22.5±2.0)年的周期性.同时也讨论了这种周期的可能机制.     

The Stability of the Light Curve of DL Cassiopeiae Between 1959–1997

A variability survey on the shape of the light curve of the classical Cepheid DL Cas has been performed on the basis of Johnson V photometry data covering about 38 years. The input parameters (mean magnitude, pulsation frequency and period, light curve amplitude, harmonics amplitudes, Fourier type structural parameters) for our study were determined through the Fourier decomposition technique applied to each data set. The analysis of the outcoming time series, using different and complementary methods, seems to indicate the constancy of these parameters within the precision limits of the available data, although the hypothesis of the presence of a low level variability cannot be excluded. The only exception is the pulsation period, which displays a possible increasing trend with a rate of 0.109 ± 0.037 s yr⁻¹. This trend may be, at least partly, an effect of the unequal precision of pulsation period estimated values, corresponding to each considered data set. This revised version was published online in July 2006 with corrections to the Cover Date.     

Star-Spots Studies for Three Short Period RS CVn-Type Binaries

Light curve analysis for three short-period RS CVn-type binaries were performed, using: a) Fourier analysis techniques for light curve changes in the frequency domain; b) photometric curve fit by means of numerical quadratures to develop theoretical light curves appropriate to RS CVn stars. The two methods were applied to the systems ER Vul, BH Vir, and UV Psc. Improved physical and geometrical parameters are found by taking the average of the results measured by the above two methods.     

Light curve and orbital elements of V 337 Aquilae

From photoelectric observations of V 337 Aql a new solution is carried out. Transit at primary eclipse in disagreement with the Wright-Dugan results is found. Both Russell-Merrill and Kitamura methods of light curve solution are used. The slight period variation and the distortions of the light curve would support the idea that a mass exchange could be in act.     

Analysis of the light curve of the magnetic CP star HD 56022

An examination of the published observational data concerning the light curves of magnetic CP stars has shown that only one star — HD 56022 — shows a light curve with a very long phase interval of light constancy. Only for this type of variability it is imaginable that the equatorial symmetry of the surface brightness distribution could be excluded. However, the analysis of the light curve of HD 56022 in the colour u of the Strömgren system has indicated that the possibly equatorial position of the small bright spot is not in contradiction to this observed curve. From the analysis in u the maximum amplitude of a light curve at another wavelength, where the curve is in counterphase to the light curve in u, can be predicted. The amplitude of such a light curve must be much smaller than 0.1 mag. From unpublished observations of HD 56022 by the satellites TD-1 A and ANS we have determined the amplitude at $LD = 155 nm, where the light curve is in counterphase to that in u, to be 0.2 mag. The consequences from the contradiction between the model and the observations in UV are discussed.