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1.
本文综述了ASCA,RXTE,Beppo SAX和XMM-NEWTON对TeV耀变体(Blazar)X射线研究的最新进展。主要集中在X射线资料的时间和光谱分析的最重要的方面,包括功率谱密度,结构函数,带间时间延迟,同步峰值能量的漂移和谱演化。对这些新结果的物理意义也进行了简要讨论。  相似文献   

2.
Blazar 的X射线谱性质   总被引:1,自引:0,他引:1  
从Donato文献中选择了一个含有69个Blazar的样本,样本中每个源有多个X射线辐射流量数据,用该样本研究了流量密度和谱指数之间的关系,以及研究了三类源(HBL,LBL,FSRQ)的红移和谱指数的分布。结果表明:对于HBLs,谱指数和流量密度之间有一个较好的反相关关系存在,而对于LBLs和FSRQs却没有相关。因此认为HBL的X射线是同步辐射所致,而LBL和FSRQ的X射线辐射较为复杂可能是同步自康普顿过程导致。HBL显示软X射线谱,而FSRQ显示硬X射线谱,LBL居中。在谱图中HBL位于近端,rSRQ位于远端,LBL居中。  相似文献   

3.
收集了18个γ射线噪BL Lac天体的X射线流量密度和γ射线流量密度,以及X射线波段(1keV)和γ射线波段(>100 MeV)的平均光谱指数,研究了它们之间的相关性.结果表明:1)X射线流量密度与γ射线流量密度在高态、低态和平均态均有较强的相关性.2)X射线波段和γ射线波段的平均光谱指数之间有较强的负相关性.3)X射线和γ射线波段的平均光谱指数与X射线和γ射线辐射流量密度在高态和平均态时均无显著的相关性.4)γ射线波段的平均光谱指数与X射线辐射流量密度的低态有较强的负相关性.X射线波段的平均光谱指数与γ射线波段的流量密度的低态之间也存在弱相关性.分析结果支持BL Lac天体的X射线和γ射线辐射可能来自同一相对论电子分布的同步辐射和同步自康普顿(SSC)辐射.  相似文献   

4.
从Fermi 3期源表(3FGL)中选择了一个含935个耀变体(blazar)的样本,包括415个平谱射电源(Flat Spectrum Radio Quasar, FSRQ), 520个蝎虎天体(BL Lac object, BL Lac),其中高同步峰BL Lac (HBL) 233个,中同步峰BL Lac (IBL) 144个,低同步峰BL Lac (LBL) 143个.研究了总样本、FSRQ、BL Lac及其子类HBL、LBL的射电1.4 GHz与γ射线在0.1、0.3、1、3、10 GeV处辐射流量密度的关系.结果显示:所有样本的射电1.4 GHz与5个波段γ射线的辐射流量都有强相关,相关系数在0.48–0.81之间,机会概率均小于10-4;对于不同的样本相关系数随着γ射线辐射频率的变化有不同的变化趋势,所有样本在5个波段的相关系数平均值随γ射线频率的增加而减小.该结果暗示,随着频率的升高, blazar的γ射线辐射主导机制在发生变化,在相同频率处,不同类型天体的辐射主导机制存在差异; HBL的γ射线辐射主要由同步自康普顿主导,而LBL的其他成份比HBL...  相似文献   

5.
从Fermi 3期源表(3FGL)中选择了一个含935个耀变体(blazar)的样本, 包括415个平谱射电源(Flat Spectrum Radio Quasar, FSRQ), 520个蝎虎天体(BL Lac object, BL Lac), 其中高同步峰BL Lac (HBL) 233个, 中同步峰BL Lac (IBL) 144个, 低同步峰BL Lac (LBL) 143个. 研究了总样本、FSRQ、BL Lac及其子类HBL、LBL的射电1.4GHz 与gamma射线在0.1、0.3、1、3、10GeV处辐射流量密度的关系. 结果显示: 所有样本的射电1.4GHz与5个波段gamma射线的辐射流量都有强相关, 相关系数在0.48--0.81之间, 机会概率均小于$10^{-4; 对于不同的样本相关系数随着gamma射线辐射频率的变化有不同的变化趋势, 所有样本在5个波段的相关系数平均值随gamma射线频率的增加而减小. 该结果暗示, 随着频率的升高, blazar的gamma射线辐射主导机制在发生变化, 在相同频率处, 不同类型天体的辐射主导机制存在差异; HBL的gamma射线辐射主要由同步自康普顿主导, 而LBL的其他成份比HBL的更复杂; FSRQ的gamma射线起源较BL Lac的复杂.  相似文献   

6.
收集了BLLac天体的有关信息作为前文(Fan&Lin1996)的补充,并在文中加入了具有喷流、具有超光速子元和具有高能射线辐射的BLLac天体表。同时在表1c中列出了BLLac天体的发射线,对偏振度与大幅光变的统计相关在相对论成束框架下给予了解释。  相似文献   

7.
射电选和X射线选BL Lacertae天体的射电性质   总被引:1,自引:0,他引:1  
收集了射电选和X射线选BL Lac天体的射电数据(包括核和延展光度), 并计算了它们的核主导系数R.研究显示: 射电选BL Lac(RBLs)天体的总射电光度是X射线选BL Lac(XBLs)天体的2个量级.详细分析得到这种差别主要是来自于核光度的差别因为延展光度差别只有1个量级.研究RBLs和XBLs的核(延展元)光度与核主导系数之间的关系, 发现延展元光度与核主导系数负相关, 而核(总)光度几乎与核主导系数没有相关.  相似文献   

8.
利用欧文斯谷射电天文台(Owens Valley Radio Observatory, OVRO) 15 GHz的观测数据,通过Jurkevich理论分析了78个耀变体样本的光变曲线,结果表明,射电源显示了显著的光变周期,范围为0.83–2.55 yr.另外,通过估算射电源光变的调制指数,发现蝎虎天体的调制指数较平谱射电类星体有更大的高斯分布峰值.  相似文献   

9.
在早期的文章中,基于耀变体(Blazar)的知识,我们预言了在射电噪活动星系核(AGN)中心10kpc范围内X射线喷流的存在。钱得拉(Chandra)卫星最近对低功率射电星系的X射线观测与我们的预言相一致。在本文中我们研究了kpc尺度喷流中的电子加速,并建议通过对强的FRⅡ射电星系中所预言的X射线喷流的钱得拉卫星的X射线的观测,来研究红的耀变体中的康普顿冷却以及在内部致密喷流和大尺度延伸喷流间环境的不同。以上的研究可以进一步检验我们的关于射电噪活动星系核中kpc尺度X射线喷流的模型。  相似文献   

10.
在早期的文章中,基于耀变体(Blazar)的知识,我们预言了在射电噪活动星系核(AGN)中心10 kpc范围内X射线喷流的存在.钱得拉(Chandra)卫星最近对低功率射电星系的X射线观测与我们的预言相一致.在本文中我们研究了kpc尺度喷流中的电子加速,并建议通过对强的FR Ⅱ射电星系中所预言的X射线喷流的钱得拉卫星的X射线的观测,来研究红的耀变体中的康普顿冷却以及在内部致密喷流和大尺度延伸喷流间环境的不同.以上的研究可以进一步检验我们的关于射电噪活动星系核中kpc尺度X射线喷流的模型.  相似文献   

11.
利用云南天文台1m光学望远镜2000~2001年对3个GeV和/或TeV γ噪Blazar天体的观测,发现γ噪类星体PKS 1510-089在R波段有一个光变时标为41min的星等变化为2.0mag的剧烈光变,这是迄今为止我们所观测到的变幅最大的一个γ噪Blazar天体短时标光变.对此光变,可估计限制光变辐射模型的一些参数,如辐射区半径R、多普勒因子δ以及吸积转化效率η等.η=59.6的值强烈预示着相对论聚束效应可较好解释γ噪Blazar天体的辐射机制.我们仔细考察了大气视宁度对光变的影响.发现对1ES 2344+514,观测到的光变与当地大气视宁度有一个弱相关,结果表明,对光变参数较小(C<5)的光变,大气视宁度引起的假光变的贡献较大,需要选择较严格的光变判据.  相似文献   

12.
13.
HST observations have shown that low-redshift 3CR radio galaxies often exhibit a point-like optical component positionally coincident with the GHz-frequency radio core. In this paper we discuss the correlation between the luminosities of the radio, optical and X-ray cores in these objects, and argue that all three components have a common origin at the base of the relativistic jets. In unified models, FR I radio galaxies should appear as dimmed, redshifted versions of BL Lac objects. We show that such models are consistent with the spectral energy distributions of the radio galaxies only if the nuclear X-ray emission in radio galaxies is inverse Compton in origin.  相似文献   

14.
We present new BeppoSAX observations of seven BL Lacertae objects selected from the 1-Jy sample plus one additional source. The collected data cover the energy range     (observer's frame), reaching ∼50 keV for one source (BL Lac). All sources characterized by a peak in their multifrequency spectra at infrared/optical energies (i.e., of the low-energy peaked BL Lac type, LBL) display a relatively flat     X-ray spectrum, which we interpret as inverse Compton emission. Four objects (two-thirds of the LBLs) show some evidence for a low-energy steepening, which is probably due to the synchrotron tail merging into the inverse Compton component around ∼     . If this were generally the case with LBLs, it would explain why the     ROSAT spectra of our sources are systematically steeper than the BeppoSAX ones     . The broad-band spectral energy distributions fully confirm this picture, and a synchrotron inverse Compton model allows us to derive the physical parameters (intrinsic power, magnetic field, etc.) of our sources. Combining our results with those obtained by BeppoSAX on BL Lacs covering a wide range of synchrotron peak frequency, ν peak, we confirm and clarify the dependence of the X-ray spectral index on ν peak originally found in ROSAT data.  相似文献   

15.
16.
We present optical identifications for a sample of 20 previously unknown X-ray/radio sources that are present both in the source catalogue of ROSAT PSPC pointed observations ( ROSAT SRC) and in the NRAO VLA Sky Survey (NVSS). The optical spectroscopy was carried out with the 2.1-m telescope at San Pedro Martir (Mexico) during 1995 April and September. We have identified 15 active galactic nuclei [including 12 broad-emission-line (FWHM >1000 km s−1) objects, one bona fide BL Lac, one BL Lac candidate and one narrow-line (FWHM < 1000 km s−1) radio galaxy] and five radio galaxies. We derive the X-ray fluxes and luminosities by analysing the PSPC exposures, and show the radio morphology from the NVSS maps.  We find that the correlation between the monochromatic X-ray luminosity at 2 keV and the core radio luminosity at 5 GHz for the radio galaxies in our sample follows that found for the 3CR radio galaxies, suggesting a possible nuclear origin for the X-ray emission in these sources. This correlation is weaker in the case of broad-line objects, indicating the presence of another (unbeamed) mechanism for the X-ray emission only weakly related to the radio emission.  相似文献   

17.
We present the results of six BeppoSAX observations of 1ES 2344+514, five of which were taken within one week. 1ES 2344+514, one of the few known TeV BL Lac objects, was detected by the BeppoSAX Narrow Field Instruments (NFI) in the range 0.1 and ≈50 keV. During the first five closely spaced observations 1ES 2344+514 showed large-amplitude luminosity variability, associated with spectacular spectral changes: in particular, the last observation found the source to be several times fainter, with a much steeper X-ray spectrum . The energy-dependent shape of the light curve and the spectral changes both imply a large frequency shift (by a factor of 30 or more) of the peak of synchrotron emission. At maximum flux the peak was located at, or above, 10 keV, making 1ES 2344+514 the second blazar (after Mrk 501) to have a synchrotron peak in the hard X-ray band. The frequency shift, and the corresponding increase in luminosity, might be caused by the onset of a second synchrotron component extending from the soft to the hard X-ray band where most of the power is emitted. Rapid variability on a time-scale of approximately 5000 s has also been detected when the source was brightest.  相似文献   

18.
It is generally believed that the high energy end of synchrotron emission, generated by the most energetic tail of relativistic electrons in the jets, account for the X‐ray emission of high‐energy peaked BL Lac objects (HBLs) and the optical emission of intermediate‐energy peaked BL Lac objects (IBLs). It is thus expected that both should show similar variability characteristics. One of the important variability parameters is the inter‐band time lag which probes the acceleration and cooling of relativistic particles responsible for the emission. The switches between soft and hard lags have been detected in the intra‐day X‐ray variability of a few HBLs, which is not the case for the intra‐day optical variability of IBLs yet. We present the results of our intra‐night optical observations for BL Lacertae, aiming at searching for hard lags of its optical variations, performed with the 80 cm telescope in fourteen nights of 2010 September‐November. Intra‐night changes of ∼0.2 mag were detected in most of nights. The intra‐night variability amplitude tends to become larger from red to blue wavelength, and the optical spectrum hardens with increasing brightness. The intra‐night variations correlate between different wavebands, but we did not find significant time lags, either soft or hard. Nevertheless, on November 2, the B band variations showed a sign of lagging the R band ones by 317±214 s. The claim of this hard lag is strongly limited by the photometric precision and time resolution. Therefore, the switches between soft and hard lags of IBLs in the optical bands needs further demonstration with more higher quality observations. (© 2016 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

19.
The results of a BeppoSAX target of opportunity (TOO) observation of the BL Lac object Mrk 421 during a high-intensity state are reported and compared with monitoring X-ray data collected with the BeppoSAX Wide Field Cameras (WFC) and the RXTE All Sky Monitor (ASM). The 0.1–100 keV spectrum of Mrk 421 shows continuous convex curvature that can be interpreted as the high-energy end of the synchrotron emission. The source shows significant short-term temporal and spectral variability, which can be interpreted in terms of synchrotron cooling. The comparison of our results with those of previous observations when the source was a factor 3–5 fainter shows evidence for strong spectral variability, with the maximum of the synchrotron power shifting to higher energy during high states. This behaviour suggests an increase in the number of energetic electrons during high states.  相似文献   

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