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1.
能谱仅反映了高能天体辐射的部分性质,而高能X射线辐射的时变可以反映致密天体的动态性质。因此,在构造高能辐射的理论模型时,既要考虑X辐射的能谱性质,也要考虑其时变性质。特别对高能天体X辐射的快速光变,一般认为其发生在致密天体附近,致密天体快速光变的研究可以揭示出致密天体附近的物理性质,因此,时变可以对X辐射模型给以很强的限制。X射线源不同能量光子到达观测者的时间差称为X射线辐射的时延。介绍了高能X辐射时变中的时延分析方法及其最新发展,综述了致密双星系统中黑洞侯选林和中子星的时延现象,并简单介绍了为解释这些现象所发展的模型,以及时延对模型的限制。  相似文献   

2.
利用最大熵谱法研究了风云二号D星≥2.0 MeV的高能电子通量的周期特性,算法以自相关模型为基础,通过对最大熵谱功率谱的分析,推测出风云二号D星高能电子通量存在13.87 d和27.8 d的周期。根据最终预报误差准则(Final Prediction Error, FPE)和赤池信息量准则(Akaike Information Criterion, AIC)确定最佳阶数,进而计算自相关模型参数,并将Levinson-Durbin和Burg算法与最大熵谱法进行比较,发现最大熵谱法在周期特性研究上存在优势。这一结果对研究地球同步轨道高能电子空间分布、预报高能电子增强事件和预警深层充电事件至关重要。  相似文献   

3.
本文讨论了有拱星壳层的AGB星的红外辐射的双黑体模型并给出了便于似合某些AGB星的红外辐射的双黑体模型并给出了便于拟合某些AGB星的红外观测数据的数学表达式,应用Taylor级数方法解决了这一复杂非线性模型拟合的困难,从而得出了一些AGB星较合理的中心星及壳层的色温度和红外能谱曲线。  相似文献   

4.
作为一种大尺度的太阳高能活动现象,日冕物质抛射(CME)的发现令人瞩目,其强烈的行星际和地球物理效应更引起了天文、空间和地球物理学家的共同关注。在本文中介绍了自CME发现以来的22年中观测和研究所取得的进展,以及它给太阳物理学带来的影响,并分析了研究工作所面临的困难和障碍,展望了CME研究的前景。  相似文献   

5.
近来我们在射电脉冲星的逆康普顿散射模型,致密星物理以及一些相关问题上做了下列几项工作:1) 对脉冲星物理中的一系列基本理论进行了较深入的研究,包括对裸奇异星比中子星更可能是射电脉冲星之起源的观点的论证。2) 进一步发展了射电脉冲星的逆康普顿散射(ICS) 模型并完成了一系列相关工作。3) 进行了脉冲星的偏振分析和有关观测工作,并用其结果对银河系磁场和旋臂结构进行了分析。4) 研究了黑洞脉冲星双星系统的一些特性,为黑洞的搜寻工作作了初步准备。  相似文献   

6.
本概述了1988年12月16日特大微波Ⅳμ型爆发的观测特征,以及由MHD调制磁流管的磁场强度产生准周期振荡,一部分高能电子被磁场俘获,作同步加速回旋辐射,产生微微汉Ⅳμ型爆发,另一部分高能电子以一定入射角喷注在磁拱上,形成螺距角各向异性的空心束分布,从而激发出电子回旋脉泽辐射(ECM),它们的垂直分量的能量便产生了尖峰辐射,叠加在Ⅳμ型爆发之上,结合怀柔的太阳磁场图,采用双极磁场模型,作出了定理  相似文献   

7.
对无线电信号在电离层中的传播路径进行了数值模拟;针对掩星观测中的五组实际卫星轨道数据(包括GPS和LEO卫星),给出了在太阳射电辐射流量(FLUX)分别为0,70,160和240等几种情况下的电离层延迟量对10.7cm波长的太阳辐射流量的响应结果;这分别对应着无太阳辐射、太阳射电辐射处于活动低谷、平静期和高峰期等几种情形。从中可以发现,掩星观测中电离层延迟量对10.7cm波长的太阳射电辐射流量的响应表现为如下特性:电离层延迟同参数FLUX的大小有明显的对应关系,即FLUX越大,则掩星观测中的电离层延迟越大;对于上升掩星情况而言,掩星观测中电离层延迟量起先逐渐增加,然后达到某一峰值,其后逐渐下降;在掩星观测的初期和中期,太阳射电辐射处于活动低谷、平静期和高峰期等几种情形之间的电离层延迟量差异都较为显著,而在掩星观测的后期,几种情形相互间电离层延迟量的差异都比较小。  相似文献   

8.
韦大明 《天文学报》1994,35(1):14-19
本文提出了关于γ爆的一种新模型,认为γ爆起源于老年中子星,老年中子星表面磁场包含两部分:一为弱的背景偶极磁场;另一为细管状局域强磁场,该模型可以同时解释γ爆能谱中回旋吸收线和高能尾巴的存在。本文用蒙特卡洛方法拟合了GB880205的能谱,与观测结构符合得比较好。  相似文献   

9.
本文概述了1988年12月16日特大微波IVμ型爆发的观测待征,以及由MHD调制磁流管的磁场强度产生准周期振荡,一部分高能电子被磁场俘获,作同步加速回旋辐射,产生微波型爆发.另一部分高能电子以一定入射角喷注在磁拱上,形成螺距角各向异性的空心束分布,从而激发出电子回旋脉泽辐射(ECM),它们的垂直分量的能量便产生了尖峰(spike)辐射,叠加在微波IVμ型爆发之上.结合怀柔的太阳磁场图,采用双极磁场模型,作出了定量计算.  相似文献   

10.
甚高能γ射线(E≥100 GeV)是全波段天文学的重要组成部分,是研究宇宙射线高能粒子的重要窗口.由于甚高能γ射线光子本身携带着重要的物理信息,对它进行研究将极大地拓展人们对宇宙演化、宇宙高能粒子、高能粒子源、高能粒子产生机制、产生环境和发射区几何形状、高能粒子之间以及高能粒子与星际介质间相互作用的认识.随着大有效面积、宽视场、较低能量阈值、较高角分辨率切仑柯夫望远镜的问世,甚高能γ射线天文学的研究取得了极大的成功,目前发现的甚高能γ射线源已经超过90个,证认了一些甚高能γ射线源的类型,包括活动星系核(AGNs)、Wolf-Rayet星、巨型分子云(GMcs)、壳层超新星遗迹(SNRs)、脉冲星风星云(PWNe)、双星系统等.介绍了甚高能γ射线的地面观测设备,并对分析方法进行评述.  相似文献   

11.
We study the multi-waveband non-thermal emission from the pulsar wind neb- ulae (PWNe) Vela X and G0.9 + 0.1 in the frame of a time-dependent model describing non-thermal radiation from the PWNe. In such a model, the relativistic wind of parti- cles driven by a central pulsar blows into the ambient medium and creates a termination shock that accelerates the particles to very high energy in a PWN. The non-thermal pho-tons in the PWN are produced both by synchrotron radiation and the inverse Compton process, with electrons coming directly from the pulsar magnetosphere and electrons be- ing accelerated at the termination shock. We apply this model to reproduce the observed multi-waveband photon spectra of Vela X and the G0.9+0.1, both of which have been detected emitting very high energy photons. Our results indicate that TeV photons are produced by the inverse Compton scattering of the high-energy electrons in the infrared photon field in both Vela X and PWN G0.9+0.1. The TeV photons from these two PWNe may have leptonic origins.  相似文献   

12.
Blazars are the only (with one or two exceptions) extragalactic objects which were detected and identified at gamma-ray energies so far. It is suspected that most of the unidentified gamma-ray sources may be the blazars as well. Because the entire electromagnetic spectrum of these objects is dominated by non-thermal radiation from relativistically moving jets, the effects such as the Klein–Nishina regime in the Compton scattering may play a major role in shaping some parts of the blazar spectrum. Within the framework of external radiation Compton model, we present how these effect influence the spectra of blazars for which the production of gamma rays is dominated by Comptonization of external radiation.  相似文献   

13.
Some massive binaries should contain energetic pulsars which inject relativistic leptons from their inner magnetospheres and/or pulsar wind regions. If the binary system is compact enough, then these leptons can initiate inverse Compton (IC) e± pair cascades in the anisotropic radiation field of a massive star. γ-rays can be produced in the IC cascade during its development in a pulsar wind region and above a shock in a massive star wind region where the propagation of leptons is determined by the structure of a magnetic field around the massive star. For a binary system with specific parameters, we calculate phase-dependent spectra and fluxes of γ-rays escaping as a function of the inclination angle of the system and for different assumptions on injection conditions of the primary leptons (their initial spectra and location of the shock inside the binary). We conclude that the features of γ-ray emission from such massive binaries containing energetic pulsars should allow us to obtain important information on the acceleration of particles by the pulsars, and on interactions of a compact object with the massive star wind. Predicted γ-ray light curves and spectra in the GeV and TeV energy ranges from such binary systems within our Galaxy and Magellanic Clouds should be observed by future AGILE and GLAST satellites and low-threshold Cherenkov telescopes, such as MAGIC, HESS, VERITAS or CANGAROO III.  相似文献   

14.
本文认为强磁场中的逆Compton散射可能是γ射线爆的主要辐射机制.其能谱是由源区质子产生的低频光子经强磁场中非热电子的Compton散射形成的.我们利用非相对论情形(B/B_(cr)≤1,hv_i/m_ec~2≤1)下强磁场中的Compton散射微分截面,导出了上述Compton散射的辐射谱公式,由此很好地拟合了典型γ射线爆GB811016的观测能谱.  相似文献   

15.
Non-thermal emission from old supernova remnants   总被引:1,自引:0,他引:1  
We study the non-thermal emission from old shell-type supernova remnants (SNRs) on the frame of a time-dependent model. In this model, the time-dependent non-thermal spectra of both primary electrons and protons as well as secondary electron/positron (e±) pairs can be calculated numerically by taking into account the evolution of the secondary e± pairs produced from proton–proton (p–p) interactions as accelerated protons collide with the ambient matter in an SNR. The multiwavelength photon spectrum for a given SNR can be produced through leptonic processes such as electron/positron synchrotron radiation, bremsstrahlung and inverse Compton scattering as well as hadronic interaction. Our results indicate that the non-thermal emission of the secondary e± pairs is becoming more and more prominent when the SNR ages in the radiative phase because the source of the primary electrons has been cut off and the electron synchrotron energy loss is significant for a radiative SNR, whereas the secondary e± pairs can be produced continuously for a long time in the phase due to the large energy-loss time for the p–p interaction. We apply the model to two old SNRs, G8.7−0.1 and G23.3−0.3, and the predicted results can explain the observed multiwavelength photon spectra for the two sources.  相似文献   

16.
Inverse Compton (IC) scattering is one of two viable mechanisms that can produce prompt non-thermal soft gamma-ray emission in gamma-ray bursts. IC requires low-energy seed photons and a population of relativistic electrons that upscatter them. The same electrons will upscatter the gamma-ray photons to even higher energies in the TeV range. Using the current upper limits on the prompt optical emission, we show that under general conservative assumption the IC mechanism suffers from an 'energy crisis'. Namely, IC will overproduce a very high energy component that would carry much more energy than the observed prompt gamma-rays, or alternatively it will require a low-energy seed that is more energetic than the prompt gamma-rays. Our analysis is general, and it makes no assumptions on the specific mechanism that produces the relativistic electron population.  相似文献   

17.
It is proposed that the spectra of so-called 'MeV blazars' can be explained in terms of previously developed models of the external Comptonization of accretion disc radiation, provided that the structure of the inner and outer parts of the accretion disc is different. The electron acceleration is saturated by the inverse Compton losses in the inner geometrically thick disc and the outer geometrically thin disc at different maximum energies; this causes the appearance of two spectral components, one strongly peaked in the MeV energy range and the other of a power-law type extending through the GeV energy range. The spectra, computed in terms of such a simple geometrical model, are in good agreement with observations of the MeV blazar PKS 0208−512. They are consistent with the transient appearance of a strong MeV peak, the power-law spectrum in the EGRET energy range, and a possible cut-off at high energies.  相似文献   

18.
This paper focuses on neutron stars (NS) of the magnetar type inside massive binary systems. We determine the conditions under which the matter from the stellar wind can penetrate the inner magnetosphere of the magnetar. At a certain distance from the NS surface, the magnetic pressure can balance the gravitational pressure of the accreting matter, creating a very turbulent, magnetized transition region. It is suggested that this region provides good conditions for the acceleration of electrons to relativistic energies. These electrons lose energy due to the synchrotron process and inverse Compton (IC) scattering of the radiation from the nearby massive stellar companion, producing high-energy radiation from X-rays up to ∼TeV γ-rays. The primary γ-rays can be further absorbed in the stellar radiation field, developing an IC  e±  pair cascade. We calculate the synchrotron X-ray emission from primary electrons and secondary  e±  pairs and the IC γ-ray emission from the cascade process. It is shown that quasi-simultaneous observations of the TeV γ-ray binary system LSI +61 303 in the X-ray and TeV γ-ray energy ranges can be explained with such an accreting magnetar model.  相似文献   

19.
A high density of massive dark objects (MDOs), probably supermassive black holes, in the centres of nearby galaxies has been inferred from recent observations. There are various indications that much of the accretion responsible for producing these objects took place in dust-enshrouded active galactic nuclei (AGNs). If so, then measurements of the intensity of background radiation and the source counts in the far-infrared and submillimetre wavebands constrain the temperature of dust in these AGNs. An additional constraint comes from the hard X-ray background, if this is produced by accretion. One possibility is that the dust shrouds surrounding the accreting AGNs are cold, about 30 K. In this event, the dusty AGNs could be some subset of the population of luminous distant sources discovered at 850 μm using the SCUBA array on the James Clerk Maxwell Telescope, as proposed by Almaini, Lawrence & Boyle. An alternative is that the dust shrouds surrounding the accreting AGNs are much hotter (>60 K). These values are closer to the dust temperatures of a number of well-studied low-redshift ultraluminous galaxies that are thought to derive their power from accretion. If the local MDO density is close to the maximum permitted, then cold sources cannot produce this density without the submillimetre background being overproduced if they accrete at high radiative efficiency, and thus a hot population is required. If the dust-enshrouded accretion occurred at similar redshifts to that taking place in unobscured optical quasars, then a significant fraction of the far-infrared background radiation measured by COBE at 140 μm, but very little of the submillimetre background at 850 μm, may have been produced by hot dust-enshrouded AGNs which may have already been seen in recent Chandra X-ray surveys.  相似文献   

20.
We describe improved modelling of the emission by dust in a toroidal-like structure heated by a central illuminating source within active galactic nuclei (AGNs). We have chosen a simple but realistic torus geometry, a flared disc, and a dust grain distribution function including a full range of grain sizes. The optical depth within the torus is computed in detail taking into account the different sublimation temperatures of the silicate and graphite grains, which solves previously reported inconsistencies in the silicate emission feature in type 1 AGNs. We exploit this model to study the spectral energy distributions (SEDs) of 58 extragalactic (both type 1 and type 2) sources using archival optical and infrared data. We find that both AGN and starburst contributions are often required to reproduce the observed SEDs, although in a few cases they are very well fitted by a pure AGN component. The AGN contribution to the far-infrared luminosity is found to be higher in type 1 sources, with all the type 2 requiring a substantial contribution from a circumnuclear starburst. Our results appear in agreement with the AGN unified scheme, because the distributions of key parameters of the torus models turn out to be compatible for type 1 and type 2 AGNs. Further support to the unification concept comes from comparison with medium-resolution infrared spectra of type 1 AGNs by the Spitzer observatory, showing evidence for a moderate silicate emission around 10 μm, which our code reproduces. From our analysis we infer accretion flows in the inner nucleus of local AGNs characterized by high equatorial optical depths  ( AV ≃ 100)  , moderate sizes  ( R max < 100 pc)  and very high covering factors (   f ≃ 80  per cent) on average.  相似文献   

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