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1.
NGC4151的长期光变行为   总被引:4,自引:0,他引:4  
樊军辉  苏成悦 《天文学报》1998,39(3):251-255
本文收集了NGC4151近90年的光学资料,并用Jurkevich分析方法对其进行了光变周期分析其光变存在一个14.04±0.8年的长周期,且该天体的谱型与源的亮度强烈相关。  相似文献   

2.
陶隽  钱伯辰 《天文学报》1998,39(2):185-192
本文利用地面光学望远镜NGC4151进行国际联测所得的结果,通过周期图方法的逐步回归方法得到了该目标目标的一些较为明显的光变周期。结果表明,NGC4151存在两个主要光变周期。一个是所有光学波段存在约14天的周期,另一个是连续谱存在30天周期,而对于Hα和Hβ则分别为24和38天的周期。  相似文献   

3.
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。  相似文献   

4.
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。  相似文献   

5.
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.  相似文献   

6.
介绍了一种用小波分析寻找BL Lac天体S5 0716+714光变周期的方法.收集了BL Lac天体S5 0716+714光学B、V、R,I四个波段较完备的观测数据,获得了10天平均的长期光变曲线.使用此光变曲线数据进行小波分析计算,结果表明小波分析方法能较好地分析和认证BL Lac天体的光变周期值.从小波变换系数实部的等值线图,可以准确证认BL Lac天体S5 0716+714有光变周期波动变化.由B,V,R,I四个波段的小波方差曲线分析发现BL Lac天体S5 0176+714有一个1160天的稳定周期,这个结果与Raiteri等人发现的3.3年周期是一致的.预测在2011年8月将有一次大的爆发.  相似文献   

7.
3C273的光学光变周期   总被引:3,自引:0,他引:3  
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.  相似文献   

8.
唐洁 《天文学报》2012,53(1):1-8
将基于多重信号分类的MUSIC谱估计算法引入BL Lac天体光变周期分析中.给出了MUSIC算法的基本原理,利用模拟信号检测了算法的频谱分辨率.从大量文献中收集了BL Lac天体S5 0716+714光学V、R、I 3个波段从1994年到2008年的有效观测数据,用MUSIC算法和平均周期图算法分别计算了它们的光变周期,发现存在两个主要光变周期:一个是(3.33±0.08)yr的周期,另一个是(1.24±0.01)yr的周期.对这两种算法的周期估计性能进行了比较,结果表明,MUSIC谱估计算法对样本长度要求较低,具有良好的分辨特性和抗噪声能力,能提高在样本长度较短情况下光变周期分析的准确性.  相似文献   

9.
从有关文献中收集了Blazar天体PKS2251+158近100年的光学观测数据,分析它的长期光变周期性.结果发现:PKS2251+158在B波段观测到的最大变化幅度是△B=2.86m.应用Jurkevich的方法分析B波段的数据,得到了一个12.39年的光变周期.在该天体中心可能有一个质量为M=8.0x105M的黑洞,并且γ辐射放大因子不小于7.2.另外,还对Jurkevich的方法进行了讨论.  相似文献   

10.
判定光变周期的一种方法   总被引:1,自引:0,他引:1  
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。  相似文献   

11.
Spectral monitoring of NGC 3516, NGC 4151, NGC 5548 and NGC 7469 has been carried out in 1986-1996 on time scales of days-months-years. In 1986-1995, the observations were made on the SAO 6-m telescope using a TV scanner with SNR about 20 in the range 4000-5200 Å (about 500 spectra). In 1996, virtually all spectra were obtained using a CCD camera with 2D and 3D spectrographs in the range 4000-7000 Å with SNR 50-100 (270 spectra). The Seyfert galaxies NGC 7469, NGC 5548, and 3C390.3 were observed in the international "AGN Watch" program by about 40 observatories around the world at optical wavelengths and by the IUE and HST in the UV. Our observations in this program demonstrated that there are no significant radial motions inside the broad line regions in NGC 4151, 3C390.3 and, possibly, in NGC 5548; that the BLR dimensions are about half those previously assumed; and that there is stratification of the BLR. The SAO 6-m observations suggest the existence of narrow satellites of the H lines during the low state of NGC 4151 in 1986-1987; new data on the narrow line region indicates the existence of an intermediate-velocity OIII component (about 2000 km/s).  相似文献   

12.
We investigate the correlation between infrared (JHKL) and optical (B) fluxes of the variable nucleus of the Seyfert galaxy NGC4151 using partially published data for the last 6 years (2008–2013). We find that the lag of flux in all the infrared bands is the same, 40±6 days, to within the measurement accuracy. Variability in the J and K bands is not quite simultaneous, perhaps due to the differing contributions of the accretion disk in these bands. The lag found for the K band compared with the B band is not significantly different from earlier values obtained for the period 2000–2007. However, finding approximately the same lags in all IR bands for 2008–2013 differs from previous results at earlier epochs when the lag increased with increasing wavelength. Examples of almost the same lag in different IR bands are known for some other active nuclei. In the case of NGC 4151 it appears that the relative lags between the IR bands may be different in different years. The available data, unfortunately, do not allow us to investigate a possible change in the lags during the test interval. We discuss our results in the framework of the standard model where the variable infrared radiation is mainly due to thermal re-emission from the part of the dusty torus closest to the central source. There is also a contribution of some IR emission from the accretion disk, and this contribution increases with decreasing wavelength.  相似文献   

13.
薛随建  程福臻 《天文学报》1998,39(2):172-184
本文利用我们所参与的1993年的国际联测光学资料,对NGC4151的BLR进行了后续Reverberation Mapping分析,其中包括a)Monte-Carlo数值模拟检验谱线光变对连续谱光变响应的最可靠的延时时标,b)用正则线性化反演方法解出BLR的转移函数。我们分析并具体解释了对NGC4151的BLR尺度的最新测量结果用1988年的测量结果存在极其显著差别的原因。  相似文献   

14.
The results of a cross-correlation analysis of the optical and X-ray light curves for eight Seyfert galaxies, NGC 5548, NGC 7469, NGC 3227, NGC 4051, NGC 4151, Mrk 509, Mrk 79, and Akn 564 and for the optical spectra of the quasar 1E 0754 are presented. In the case of the galaxies NGC 5548 and NGC 7469, the maximum values of cross-correlation coefficients for optical and X-ray variations proved to be high (0.73 and 0.79, respectively). The lag time, determined from the maximum of cross-correlation function, is 2.800 ?1.58 +3.12 days for NGC 5548 and 0.6 ?4.3 +0.9 days for NGC 7469. This result favors downscattering of the X-ray emission into the optical range (direct Compton effect) for NGC 5548 and NGC 7469. In addition to the main maximum, which corresponds to the lag of the optical flux variations behind the X-ray flux, six objects (excluding Akn 564 and NGC 4151) show the wings in the intervals of cross-correlation functions that correspond to the time lags of X-ray emission behind the optical emission of approximately 10 days. A method of determining the masses of central black holes in AGNs through spectral line widths is presented; with this method the mass of the central black hole in the quasar 1E 0754 was found (M BH = 1.01 × 108 M sun). The position of the quasar 1E 0754 in the mass-luminosity diagram meets the position of other NLS 1 galaxies.  相似文献   

15.
Numerous U and V magnitude measurements were performed for the nucleus of the Seyfert galaxy NGC 4151 at the Crimean Laboratory of the SAI (Moscow University) in 1994–2005. Adding them to the previous data for 1968–1997 has led to a substantial increase in the confidence level of the light variations in NGC 4151 with a stable period of P G = 160.0108(7) min and a mean amplitude of 0.007 U mag (in the “active” state of the nucleus). The period of NGC 4151 agrees well with the period of 160.0101(15) min found previously in the oscillations of the Sun. It is treated as the period of a “coherent cosmic oscillation” independent of redshift z or as the period of “free cosmic vibrations” of the hydrogen atom, the main element of the Universe. The period and initial phase of the P G oscillation have been constant for 38 years of NGC 4151 observations. The new astrophysical phenomenon appears to be closely related to the quantum nonlocality of photons and is of particular interest in physics and cosmology.  相似文献   

16.
We search for a direct signature of discrete 'clouds' in the broad-line region (BLR) of the Seyfert galaxy NGC 4151. For this purpose we apply cross-correlation (CC) analysis to a high-resolution Keck spectrum of the galaxy. No such signature is found in the data. In order for cloud models to be compatible with this result, there must be at least ∼3×107 emitting clouds in the BLR, where the limit is based on simulation of a homogeneous cloud population. More realistic distributions increase the lower limit to above 108. These numbers are an order-of-magnitude improvement on our previous limit from Mrk 335, where the improvement comes from higher signal-to-noise ratio (S/N), broader lines and refined simulations. Combined with the predicted upper limit for the number of emitting clouds in NGC 4151 (106–107), the derived lower limit puts a strong constraint on the cloud scenario in the BLR of this object. Similar constraints can be placed on models where the emission originates in streams and sheets. Thus, this investigation suggests that the broad emission lines (BELs) in NGC 4151, and by extension in all AGNs, are not made of an ensemble of discrete independent emitters.  相似文献   

17.
In the frame of the Starburst model, we show that the stellar processes expected to occur during the evolution of a metal rich massive stellar cluster can reproduce the observed optical light curves of the Seyfert 1 galaxies NGC 4151 and NGC 5548.  相似文献   

18.
Astronomy Letters - The results of UBVRIJHK photometry for the type II-P supernova SN 2018aoq in NGC 4151 obtained from April 4, 2018, to January 14, 2019, with several telescopes, including the...  相似文献   

19.
Photographic observations of the nucleus of the Seyfert galaxy NGC 4151, carried out during the last seven years, are reported. The object shows irregular variations between photographic magnitudes 11.2 and 13.0.  相似文献   

20.
Photometric observations of the nucleus of NGC 4151 obtained in a period of 16 nights in April 1990 in the 5672 Å continuum and theU-band have clearly shown that the nucleus has entered into an active phase and its energy output is still rising.  相似文献   

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