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1.
本文提出一个持续供能的喷流—激波模型来解释视超光速射电节点频谱演化的普遍特性.理论计算指出,射电爆发频谱的反转频率νm和频谱极大流量Sm之间的关系具有典型的3阶段演化方式,并且与类星体3C345中观测到的视超光速节点C4的演化行为相当好地符合.令Sm∝ν,则在上升阶段ζ≤3;在平坦变化阶段ζ≈0,而在衰减阶段ζ≈1.爆发幅度和流量极大的迟后时间对频率的关系△Smax(ν)和△t(ν),都具有Blazar天体中观测到的射电爆发的普遍形式.本文提出的激波模型,考虑到驱动气体的持续注入和激波后等离子体的绝热膨胀.因此提供了对相对论喷流中激波形成和演化的物理原因更深入的理解.并对Blazar天体中视超光速节点频谱演化提出了新的解释.  相似文献   

2.
为了解释Blazar天体射电爆发的普遍演化特性,本提出一个持续注入的喷流模型。假定在喷流基底上以相对论性速度持续地注入相对论等离子体(由磁场和相对论电子组成)。这一等离子体在沿喷流向外运动时经受绝热膨胀损耗。理论计算表明,射电爆发的频谱演化具有Valtaoja等人所建议的典型的3阶段演化形式。它们非常好地重现了Blazar天体中观测到的射电爆发的普遍行为。  相似文献   

3.
VLBI观测表明,TeV伽马射线Blazar(耀变体)的喷流运动视速度远小于MeV/GeV伽马射线Blazar,然而TeV伽马射线辐射流量的快速变化却要求这些Blazar的相对论喷流速度与MeV/GeV Blazar的相当.对于这一矛盾,目前有多种解释.为了检验这些模型,我们收集了VLBI对Blazar喷流运动的监测数据,样本包括86个FSRQs(平谱射电类星体)、22个BL Lac天体,共108个Blazar;从统计上研究了,该样本中各Blazar最大视速度喷流节点的位置与射电光度相关关系.结果表明,Blazar最大视速度喷流节点的位置与射电光度有较强的相关关系,随着Blazar射电光度的减小,喷流中最大视速度VLBI节点的位置到VLBI核的距离逐渐变小.这意味着,TeV伽马源(低光度Blazar)的喷流减速区距离VLBI核较近,喷流从高能辐射区到VLBI可分辨尺度已经减速,支持减速喷流模型对TeV伽马射线Blazar上述矛盾的解释.  相似文献   

4.
本文对相对论电子的辐射性质、能谱演化和加速机制等进行了简要的介绍。同时,对相对论电子在高能天体中的辐射作用和特性进行了简要的综述。本文给出了相对论电子在Blazar天体的射电辐射机制、光变机制、BL Lac天体的辐射机制以及γ暴的辐射机制等方面的应用研究成果。1、提出了相对论电子的光学薄同步辐射模型:解释Blazar天体的射电平谱:Blazar中心体的剧烈活动,使射电辐射区处于等离子体湍动状态,其中的相对论电子在湍动等离子体波的二交费米加速、激波加速、辐射损失、粒子逃逸和辐射区的绝热减速等物理过程作用下,形成较平的能谱,产生射电平谱。2、提出了新的Blazar天体光变模型:当Blazar天体爆发时,中心天体产生大量的相对论电子,注入喷流中;相对论电子产生同步辐射,并不断损失能量和逃逸辐射区,使它们的能谱快速变化,引起辐射发生快速光变。3、给出了BL Lac天体的等离子体反应堆模型:大量相对论电子从中心天体注入周围的等离子体反应堆中,通过同步辐射快速损失能量,同时这些电子同步吸收反应堆中不透明的光子,产生一个稳定、各向同性的幂律分布,其谱指数为γ=3;然后,这些相对论电子通过等离子体反应堆的爆发或其表面扩散过程逃逸出来,辐射低频的同步辐射。模型解释了BL Lac天体的高频辐射表现出快速的谱变化性质,即流量减小时谱变陡。4、提出了相对论电子的内激波加速模型,解释γ暴的尖峰光变特性:在γ暴产生的相对论运动的壳层中,有内激波产生;激波在壳层中传播,耗散壳层的运动能,使其中的部分电子加速成为相对论电子。然后,这些电子通过同步辐射产生观测到的γ辐射。模型认为,γ暴中的每个尖峰辐射是一对内激波加速相对论电子的辐射过程,复杂的γ暴光变曲线是多对内激波辐射过程的叠加。  相似文献   

5.
钱善Jie 《天文学报》1997,38(3):239-249
本文讨论Blazar天体中光学射电大爆发频谱演化的理论模型.考虑沿喷流传播的相对论性激波所注入或加速的相对论性电子,受到康普顿、同步辐射和绝热膨胀三种损耗,并计及相对论电子能谱的高能截断.假定喷流轴线与观测者方向构成很小角度.文中给出了大爆发频谱三阶段连续演化的特性,即康普顿阶段,同步辐射阶段和绝热膨胀阶段的爆发特性.频谱演化用(Sm-vm)关系表达(见图2,图中Sm为频谱反转流量,vm为反转频率),它与一些Blazar天体中观测到的典型形式相符合.  相似文献   

6.
收集了47个Blazar天体的短时标光变资料,估算了中心天体质量和不同波段辐射区域,并对估算结果作了统计分析,发现Blazar天体中心黑洞质量在10~7M_☉到10~(10)M_☉之间,BL Lac天体与平谱射电类星体中心黑洞质量有很大差异,平谱射电类星体中心黑洞质量大于BL Lac天体中心黑洞质量;红外波段和γ射线波段辐射区域大小相似.同时,利用收集到Blazar天体的热光度分析了Blazar天体热光度与短时标光变之间的关系,证实了射电选BL Lac(RBL)天体和平谱射电类星体(FSRQs)的辐射是强成束的,但相对论聚柬效应对X射线选BL Lac(XBL)天体的辐射影响较小.  相似文献   

7.
本提出一个持续供能的喷流-激波模型来解释视超光速射电节点频谱演化的普遍特性。理论计算指出,射电爆发频谱的反转频率Vm和频谱极大流量Sm之间的关系具有典型的3阶段演化方式,并且与类星体3C345中观测到的视超光速节点C4的演化行为相当好地符合。令Sm∝Vm^ζ,则在上升阶段ζ〈 ̄-3;在平坦变化阶段ζ≈0,而在衰减阶段ζ≈1,爆发幅度和流量极大的迟后时间对频率的关系ΔSmax(V)和Δt(V),都  相似文献   

8.
文中对6颗Blazar天体15年间的大量准同时性观测数据进行了处理分析,获得了长期的光变曲线和色指数变化曲线。对比分析光变曲线和色指数变化曲线,对色指数和亮度做相关分析,得出Blazar天体的光变包括长期的单色光变和有颜色变化的短期爆发两种成份,由光变的颜色差异我们提出引起Blazar天体光变的物理机制可能是几何效应调制的激波喷流模型。  相似文献   

9.
本文研究了Blazar天体的辐射性质,提出一种新的喷流模型,即具有幂律分布的极端相对论电子团从中心核注入喷流等离子体中,它在一定的注入速度下,不仅能在喷流等离子体中激发等离子体湍动,产生电磁波的相干辐射,而且能产生强的同步辐射。利用等离子体的弱湍理论,我们研究了极端相对论电子团在喷流等离子体中的辐射过程,并详细研究了它在解释Blazar天体辐射特性中的应用,本文认为,Blazar天体的不稳定辐射与极端相对论电子团的无规注入、喷流等离子体的物理环境瞬息变化有关。Blazar中快速变化的辐射偏振角摆动。产生于相对论电子团在湍动等离子体中的同步辐射过程。另外,X选和射电选的BLLac天体之间的区别取决于喷流等离子体的运动状态和物理环境。  相似文献   

10.
耀变体(Blazars)的亮温度与黑洞喷流能量和吸积率有重要关系。搜集了53个耀变体源样本,包括22个蝎虎天体(BL Lacs)和31个平谱射电类星体(Flat Spectrum Radio Quasars,FSRQs),研究了耀变体亮温度与黑洞喷流能量的分布,并对子类中亮温度与黑洞喷流能量的相关性进行了讨论。研究结果表明:(1)蝎虎天体与平谱射电类星体的亮温度与黑洞喷流能量的分布存在明显差异,这可能与蝎虎天体与平谱射电类星体的内禀性质有关,也可能与其有无发射线及发射线的强弱有关;(2)蝎虎天体的亮温度与黑洞喷流能量之间的相关性较强,亮温度可以在一定程度上描述蝎虎天体的黑洞喷流能量,亮温度大的蝎虎天体喷流携带的能量也较大;(3)平谱射电类星体的亮温度与黑洞喷流能量之间有弱相关性,平谱射电类星体的亮温度不能清楚地描述黑洞喷流能量,黑洞喷流能量受亮温度影响较小,平谱射电类星体的黑洞喷流能量可能受到其他因素的影响;(4)耀变体的亮温度与黑洞吸积率之间有弱的相关性。  相似文献   

11.
Active galactic nuclei(AGNs)have two major classes,namely radio loud AGNs and radio quiet AGNs.A small subset of the radio-loud AGNs is called blazars,which display extreme observational properties,such as rapid variability,high luminosity,high and variable polarization,and superluminal motion.All of those observational properties are probably due to a relativistic beaming effect with the jet pointing close to the line of sight.Observations suggest that the orientation can be expressed by a core-dominance p...  相似文献   

12.
During the period of 1991–1993 two strong high energy γ-ray flares were observed by the Compton Gamma Ray Observatory in the flat spectrum radio source PKS 0528+134. They were associated with strong mm-radio outbursts with a few months time-delays. In this paper the spectral energy distributions (SED) of the radiations in the γ-hand X-ray and the IR-optical bands are analysed. It is shown that the high energy γ-ray radiation may be due to the inverse Compton scattering of the ambient UV and soft X-ray photons by the relativistic electrons in the jet. Basing on the comparison between the properties of the synchrotron radiation of the γ-ray source and the spectral evolution of the mm-radio outbursts, the evolutional relationship between the γ-ray emitting blobs and the mm-radio emitting blobs is discussed.  相似文献   

13.
We collect a sample of 51 Fermi-detected gamma-ray loud blazars with known radio Doppler factors and study properties of the Doppler factors of blazars at optical,X-ray and gamma-ray bands.A basic assumption is that the emission from the radio to gamma-ray bands of the blazars are produced by the nonthermal radiation of accelerated particles in a jet.Our results show that (1) the Doppler factors of blazars are a function of frequency,with the Doppler factor decreasing with frequency from the radio to X-ray ...  相似文献   

14.
We estimate the power of relativistic, extragalactic jets by modelling the spectral energy distribution of a large number of blazars. We adopt a simple one-zone, homogeneous, leptonic synchrotron and inverse Compton model, taking into account seed photons originating both locally in the jet and externally. The blazars under study have an often dominant high-energy component which, if interpreted as due to inverse Compton radiation, limits the value of the magnetic field within the emission region. As a consequence, the corresponding Poynting flux cannot be energetically dominant. Also the bulk kinetic power in relativistic leptons is often smaller than the dissipated luminosity. This suggests that the typical jet should comprise an energetically dominant proton component. If there is one proton per relativistic electrons, jets radiate around 2–10 per cent of their power in high-power blazars and 3–30 per cent in less powerful BL Lacs.  相似文献   

15.
Superluminal Motion and Polarization in Blazars   总被引:3,自引:0,他引:3  
A relativistic beaming model has been successfully used to explain the observed properties of active galactic nuclei (AGNs). In this model there are two emission components, a boosted one and an unbeamed one, shown up in the radio band as the core and lobe components. The luminosity ratio of the core to the lobe is denned as the core-dominance parameter (R = LCore/LLobe). The de-beamed radio luminosity (Ldbjet) in the jet is assumed to be proportional to the unbeamedluminosity (Lub) in the co-moving frame, i.e., f = Ldbjet/Lub, and f is determined in ourprevious paper. We further discuss the relationship between BL Lacertae objects (BLs) and flat spectrum radio quasars (FSRQs), which are subclasses of blazars with different degrees of polarization, using the calculated values of the ratio f for a sample of superluminal blazars. We found 1) that the BLs show smaller averaged Doppler factors and Lorentz factors, larger viewing angles and higher core-dominance parameters than do the FSRQs, and 2) that in th  相似文献   

16.
The central engine causing the production of jets in radio sources may work intermittently, accelerating shells of plasma with different mass, energy and velocity. Faster but later shells can then catch up slower earlier ones. In the resulting collisions shocks develop, converting some of the ordered bulk kinetic energy into magnetic field and random energy of the electrons which then radiate. We propose that this internal shock scenario , which is the scenario generally thought to explain the observed gamma-ray burst radiation, can also work for radio sources in general, and for blazars in particular. We investigate in detail this idea, simulating the birth, propagation and collision of shells, calculating the spectrum produced in each collision, and summing the locally produced spectra from those regions of the jet which are simultaneously active in the observer's frame. We can thus construct snapshots of the overall spectral energy distribution, time-dependent spectra and light curves. This allows us to characterize the predicted variability at any frequency, study correlations between the emission at different frequencies, specify the contribution of each region of the jet to the total emission, and find correlations between flares at high energies and the birth of superluminal radio knots and/or radio flares. The model has been applied to reproduce qualitatively the observed properties of 3C 279. Global agreement in terms of both spectra and temporal evolution is found. In a forthcoming work, we will explore the constraints that this scenario sets on the initial conditions of the plasma injected in the jet and the shock dissipation for different classes of blazars.  相似文献   

17.
We report on the optical color variability of a sample of 24 blazars, consisting of nine flat spectrum radio quasars(FSRQs) and 15 BL Lacertae objects(BL Lacs), on timescales of years using simultaneous V-and R-band observations observed by the Kanata telescope at Higashi-Hiroshima Observatory.The correlations between color indices V-R and magnitudes reveal that 11 BL Lacs and one FSRQ exhibited significant(i.e., r 0.2 and P 0.01) bluer-when-brighter(BWB) trend and two FSRQs followed the redder-when-brighter(RWB) tend, indicating a possibility that the BWB chromatic trend is dominant for BL Lacs and the RWB trend is especially found in FSRQs, which has been presented occasionally in different samples of blazars.The superpositions of the red emission component from the Doppler-boosted relativistic jet and the blue component arising from the accretion disk might be a possible interpretation for the long-term color behaviors.  相似文献   

18.
On the basis of issues raised by observations of BL Lac objects and the qualitative jet model proposed by Bakeret al. in 1988, we have been led to consider the quantitative role of coherent, stimulated emission in jets and construct a new jet model of blazars in which a relativistic electron beam with an axial symmetric, power-law distribution is injected from the central engine into the jet plasma. We study quantitatively the synchrotron emission of the relativistic electron beams. Using the weak turbulent theory of plasma, we discuss the interaction between relativistic electron beams and jet plasma, and the roles of stimulated emission. The main results are:
  1. The synchrotron emission increases sensitively with the increase of the angle between the direction of the beam and the magnetic field. When the direction of the beam is vertical to the magnetic field, the synchrotron emission reaches its maximum, i.e. the emitted waves are beamed in the direction of the jet axis. We suggest that radio selected BL Lac objects belong to this extreme classification.
  2. The synchrotron emission of the relativistic beam increases rapidly with the increase of the Lorentz factor of the relativistic electron,γ, whenγ ≤ 22.5, then decreases rapidly with increase ofγ.
  3. The stimulated emission also increases with increasing Lorentz factorγ of the relativistic electrons whenγ ≤ 35 and then decreases with the increasingγ. The maximum stimulated emission and the maximum synchrotron emission occur at different frequencies. Stimulated emission is probably very important and reasonable flare mechanism in blazars.
  4. The rapid polarization position angle (PA) swings may arise from the interaction between the relativistic electron beam and the turbulent plasma.
  相似文献   

19.
The magnetic field in an accretion disk is estimated assuming that all of the angular momentum within prescribed accretion disk radii is removed by a jet. The magnetic field estimated at the base of the jet is extrapolated to the blazar emission region using a model for a relativistic axisymmetric jet combined with some simplifying assumptions based on the relativistic nature of the flow. The extrapolated magnetic field is compared with estimates based upon the synchrotron and inverse Compton emission from three blazars, MKN 501, MKN 421 and PKS 2155-304. The magnetic fields evaluated from pure synchrotron self-Compton models are inconsistent with the magnetic fields extrapolated in this way. However, in two cases inverse Compton models in which a substantial part of the soft photon field is generated locally agree well, mainly because these models imply magnetic field strengths consistent with an important Poynting Flux component. This comparison is based on estimating the mass accretion rate from the jet energy flux. Further comparisons along these lines will be facilitated by independent estimates of the mass accretion rate in blazars and by more detailed models for jet propagation near the black hole.  相似文献   

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