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1.
CygX-1 X辐射的功率谱   总被引:1,自引:1,他引:0  
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.  相似文献   

2.
本文介绍了云南天文台一米望远镜附属的一台低色散光谱仪实验装置,介绍了该装置的设计原理、系统结构参数及试观测情况,并讨论了存在的问题和解决问题的设想。我们已用该装置观测到19m左右的具有大红移的类星体光谱。该类低色散光谱仪,将为我国星系研究工作者提供实测条件。  相似文献   

3.
研究了Fermi-LAT第4期目录中的射电星系(Radio galaxy, RDG)以及窄线型赛弗特星系1 (Narrow-line Seyfert 1, NLSY1)的γ射线流量分布特征及均方根-流量(RMS-Flux)的线性关系。基于这两类活动星系核的γ射线流量数据处理,用高斯函数和对数正态函数对其流量分布进行了拟合。通过K-S检验(Kolmogorov-Smirnov test)、S-W检验(Shapiro-Wilk test)及约化卡方(Reduced χ2)发现,射电星系及窄线型赛弗特星系1的分布都更加符合对数正态分布而非高斯分布,这表明其光变可能具有非线性和乘法性质。此外,还分别对这两类源的两种不同分组的均方根-流量关系进行了线性拟合,发现了均方根-流量有极强的线性相关性且斜率都为正。  相似文献   

4.
用于2.4m望远镜的网络气象站   总被引:1,自引:1,他引:0  
在进行天文观测时,天气因素的影响是很大的,为适应天文观测技术发展的要求,在2.4m镜附近需要建立一个网络气象站,一方面可以对天气状况实时监测,另一方面其他设备可以从网上查询并使用这些数据,以满足2.4m望远镜必须要有气象状况输入才能正常地在RoboticMode下工作的要求。文中介绍了1 wirenet气象站的原理以及软硬件设计。  相似文献   

5.
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   

6.
本文研究了1986-1988年美国喷气推进实验室、法国地球动力学中心和上海天文台用激光测月资料推算的UT1-UTC值,并与国际地球自转参数服务给出的UT1-UTC值作比较,得到各分析中心推算UT1-UTC值的内符和外符。  相似文献   

7.
董爱军  王建成  薛力 《天文学报》2006,47(3):231-246
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   

8.
利用′tHooft的边界条件和“准周期”边界条件分别求解了1+1维黑洞背景时空中的KleinGordon方程和Dirac方程,并计算了相应的玻色子熵与费米子熵,发现它们具有同一发散形式,两者仅相差一个系数  相似文献   

9.
1985年9月22日,我们用空间硬X射线望远镜HAPI-2,在我国的高空气球上,对天鹅座X-1进行了观测,望远镜几何面积为140cm~2,观测能区20—200keV,空间定向精度±0.2°。获得的硬X射线能谱陡,总辐射能流LX~1.0×1~(37)erg/sec,低于常规态。本文将介绍望远镜的性能和观测过程,能谱分析的结果,并对当时天鹅座X-1可能的“态”进行讨论。  相似文献   

10.
云南天文台1m望远镜终端之一的暗天体分光仪和照相机具有4种运行模式:缩焦照相机、无缝多目标光谱仪、有缝光谱仪和星冕仪。这4种运行模式能在几分钟的时间内相互转换,高效快速和灵活方便。该仪器的光学质量优秀,光学系统消像差,特别是消色差。由于光学系统消色差,所成像的低色散光谱在404.6~766.5nm全波段尖锐平直。在多色测光时,各测光波段的像面位置不变,同时兼有大视场的优点,可提高测光精度和测光效率。  相似文献   

11.
1 INTRODUCTIONStudying short time scale variability of the X-ray emission of blaCk-hole systems and lowmass X-ray binaries is an importal approach to understanding the emitting region and elinssionmechanism of high-energy photons. The time-averaged spectra of hard X-rays from Cyg X-1and other black-hole candidates are relatively well explained in terms of a simple model: hardX-rays result from the Comptonization of soft photons in a hot electron cloud of constattemperature and optical d…  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 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   

13.
Hercules X‐1 is an x‐ray binary with a 1.7 day orbit and which exhibits a regular 35‐day intensity cycle, which comes in two types: 0.2 orbital phase turn‐on and 0.7 phase turn‐on. The cycle is well measured by the RXTE/ASM and is caused by a sequence of occultations by the inner and outer edges of the accretion disk. In addition to the 35‐day x‐ray cycle, the accretion disk shadows the companion star HZ Her to give the regular and well known optical modulation, and gives a modulation of the EUV emission from the system. The x‐ray modulation is most precisely measured and best for determination of the disk shape. Here disk and emission region models are used to derived the disk shape from the 0.2 turn‐on cycles and compared to a previous derivation based on 0.7 turn‐on cycles. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

14.
利用线性状态空间模型(Linear State Space Model-LSSM),将 Cyg X-1的功率谱分解为LSSM产生的模型功率谱和剩余功率谱两部分.集中分析剩余功率谱,结果显示, Cyg X-1在低/硬态、转换态和高/软态三种状态的剩余功率谱有着不同的结构特征.其中高/软态和低/硬态的剩余功率谱存在一个宽峰结构,中心频率分别为~ 8 Hz和~ 5 Hz,低/硬态的剩余功率诺在~ 0.07 Hz达到极大;转换态的剩余功率谱有双峰结构,其中心频率分别在~0.5—4Hz和~5—11Hz,与我们以前分析的 QPO的中心频率很接近,说明 QPO与线性状态空间所要求的自回归模型可能属于不同的物理过程.与总功率谱比较,剩余功率谱对谱的变化部分(例如QPO、截断频率等)更为敏感,本文对剩余功率谱中谱峰变化的原因做了初步的探讨.  相似文献   

15.
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   

16.
一些作者提出Her X-1的35天开关周期是由中子星的自由进动引起的。对这个模型我们进行了理论计算,并将理论结果和观测资料进行了比较,我们发现: (1)Hcr X-1的35天周期的光变曲线的理论值与观测(Jones & Forman,1976)不符。 (2)在这个模型中脉冲宽度和强度随35天周期有很大的变化(见图4和图5),也与观测不符(如Gruber等人1980年的观测)。 (3)Parmar等人(1985)报道他们没有发现预期的Her X-1的X射线辐射35天周期的变化,这也同中子星自由进动的模型不一致。 Pravdo等(1977)建议观测到的X射线脉冲是由产生于中子星表面附近的、对称的辐射束经汤姆逊散射而形成。我们用强磁场中的汤姆逊散射理论所作的分析表明,该模型可以较好地与观测相符。  相似文献   

17.
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   

18.
It has been suggested that the 35 day clock mechanism of Her X-1 is caused by the precession of the neutron star. We made calculations for this model. Comparing our calculated results with observations we find:
1. (1) The theoretical light curve over the the 35 day cycle does not agree with the observed curve by Jones and Forman (1976).

2. (2) The change of pulse width and intensity with the 35 day phase is large in the model, seemingly disagreeing with the observations (e.g., Gruber et al. 1980).

3. (3) Parmer et al. (1985) reported that they did not see the expected 35 day variation in X-ray intensity expected in the model.

Pravdo et al. (1977) suggested that the observed X-ray pulses were formed by Thomson scattering of symmetric radiating beams generated near the surface of the neutron star. Our analysis based on the theory of Thomson scattering in strong magnetic fields shows that this model agrees well with the observations.  相似文献   


19.
We have obtained high time resolution (seconds) photometry of LMC X-2 in 1997 December, simultaneously with the Rossi X-ray Timing Explorer ( RXTE ), in order to search for correlated X-ray and optical variability on time-scales from seconds to hours. We find that the optical and X-ray data are correlated only when the source is in a high, active X-ray state. Our analysis shows evidence for the X-ray emission leading the optical with a mean delay of <20 s. The time-scale for the lag can be reconciled with disc reprocessing, driven by the higher-energy X-rays, only by considering the lower limit for the delay. The results are compared with a similar analysis of archival data of Sco X-1.  相似文献   

20.
We describe a new method to estimate the mass of black holes in Ultraluminous X-ray Sources (ULXs). The method is based on the recently discovered 'variability plane', populated by Galactic stellar-mass black-hole candidates (BHCs) and supermassive active galactic nuclei (AGNs), in the parameter space defined by the black-hole mass, accretion rate and characteristic frequency. We apply this method to the two ULXs from which low-frequency quasi-periodic oscillations have been discovered, M82 X-1 and NGC 5408 X-1. For both sources we obtain a black-hole mass in the range  100–1300 M  , thus providing evidence for these two sources to host an intermediate-mass black hole.  相似文献   

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