同步自吸收对Gamma射线暴余辉的影响

考虑同步自吸收效应后,讨论了Gamma射线暴余辉的谱并展示了Gamma射线暴GRB970508余辉在光学波段的光变曲线,尽管光学余辉很复杂,所得到的结果仍然与观测结果符合的很好,因此不管是在火球＋激波模型还是在喷流模型中,都应该全面地研究同步自吸收效应和内部能源机制,以使理论计算更好的拟合观测到的光变曲线。     

γ射线暴火球模型的光学余辉辐射

按照γ射线暴火球模型的动力学演化规律,利用相对论电子在磁场中作同步加速辐射时谱分布的特点,用求峰值频率辐射的方法,计算了γ射线暴红光波段余辉辐射流量随时间的变化与γ射线暴GRB970228的观测结果比较,符合甚好,说明同步加速辐射是γ射线暴余辉主要的辐射机制,也进一步证明了火球模型的正确。     

柱形喷流中考虑同步自吸收的伽玛射线暴余辉

在统一动力学模型和柱形喷流模型的基础上,用四阶的龙格库塔法求解动力学演化的方程,并考虑同步加速辐射中的自吸收效应,用数值计算方法得到GRBs余辉随时间t演化关系.     

对含自吸收热等离子体中同步加速辐射的研究

对含有磁场的相对论热等离子体的同步加速辐射，考虑等离子体的自吸收，求解辐射转移方程，得到等离子体表面向外的同步加速辐射的辐射强度。     

中心有脉冲星的γ暴970228火球模型

重点讨论了中心有脉冲量生的γ射线暴火球模型，假定在火球的中心有一强磁场的毫秒级脉冲星，改革以往文献中的能量转化方程，计算出GRB970228的辐射流，与观测结果符合的很好，自然解释了GRB970228余辉的光变曲线特征。     

一种对伽玛暴瞬时谱的新解释

研究了幂律分布电子的同步曲率辐射在伽玛暴（gamma-ray burst,GRB）的物理条件下的表现,并用同步曲率辐射机制代替同步辐射来解释伽玛暴的瞬时谱,尤其是那些出现拐点和高能过剩的谱,还拟合了几个实际的有拐点和高能过剩的伽玛射线暴的瞬时谱.从中可以看出,同步曲率辐射机制对整个瞬时谱能够做出统一和合理的解释.在对高能过剩部分的解释中,同步曲率辐射机制不需再人为引入任何其他机制,因此可调参数少.此外,该机制还能对发射区磁场给出更加详细的描述,尤其是对磁场的曲率半径有了严格的约束,因此对磁场的形成机制给出严格的限制,支持了磁场产生于激波的理论模型.将来对更高能部分的更精细的观测将能够对我们的模型进行进一步检验.最后用同步曲率辐射对GRB 941017的谱的瞬时谱部分的演化进行了拟合和讨论.     

弯曲磁场中相对论性电子辐射的自吸收性质及等离子体影响

根据同步曲率辐射理论，论文推导了真空中和等离子体中弯曲磁场下相对论性电子辐射的自吸收系数，发现真空中同步曲率辐射与同步辐射一样没有负吸收放大作用，而等离子体对辐射谱和自吸收性质有重大影响，存在脉泽放大效应。这些结果有可能对宇宙中多种射电源的射电高亮温度等问题提供可能的解释。     

各向同性火球中考虑同步自吸收的伽玛暴余辉

基于Huang,Y．F．等人的统一动力学模型，研究了星际介质环境下各向同性火球所抛壳层的动力学量随时间的演化，考虑了同步自吸收效应，用数值计算方法得到不同频率下随时间演化的伽玛暴余辉，同柱状喷流下伽玛暴余辉比较，得出相应结论．     

相对论热等离子体的同步加速辐射

利用克希霍夫定律及光深条件等物理上的考虑，对具有磁场的相对论热等离子体采用一种简化的方法来处理包含自吸收的同步加速辐射，求得辐射率的表达式．     

蟹状星云中γ射线的辐射机制

根据蟹状星云中γ射线的观测数据拟合谱,对γ射线的辐射机制进行了分析,通过同步加速吸收的加速机制使电子得到产生γ射线的能量,定性确定了辐射γ射线的电子能量的上限,由观测谱推断高能γ射线是逆康普顿散射机制产生的,并由此确定了不同能量段的γ射线发自星云不同的区域。     

Structure in the early afterglow light curve of the gamma-ray burst of 29 March 2003

Gamma-ray bursts (GRBs) are energetic explosions that for 0.01-100 s are the brightest gamma-ray sources in the sky. Observations of the early evolution of afterglows are expected to provide clues about the nature of the bursts, but their rapid fading has hampered such studies; some recent rapid localizations of bursts have improved the situation. Here we report an early detection of the very bright afterglow of the burst of 29 March 2003 (GRB030329). Our data show that, even early in the afterglow phase, the light curve shows unexpectedly complicated structures superimposed on the fading background.     

Evolution of the polarization of the optical afterglow of the gamma-ray burst GRB030329

The association of a supernova with GRB030329 strongly supports the 'collapsar' model of gamma-ray bursts, where a relativistic jet forms after the progenitor star collapses. Such jets cannot be spatially resolved because gamma-ray bursts lie at cosmological distances; their existence is instead inferred from 'breaks' in the light curves of the afterglows, and from the theoretical desire to reduce the estimated total energy of the burst by proposing that most of it comes out in narrow beams. Temporal evolution of the polarization of the afterglows may provide independent evidence for the jet structure of the relativistic outflow. Small-level polarization ( approximately 1-3 per cent) has been reported for a few bursts, but its temporal evolution has yet to be established. Here we report polarimetric observations of the afterglow of GRB030329. We establish the polarization light curve, detect sustained polarization at the per cent level, and find significant variability. The data imply that the afterglow magnetic field has a small coherence length and is mostly random, probably generated by turbulence, in contrast with the picture arising from the high polarization detected in the prompt gamma-rays from GRB021206 (ref. 18).     

The Fabrication and Properties of a Blue Long Afterglow Phosphor

1Introduction　SincethefindingoflongafterglowphosphorofZnS :Cuintheearly 2 0thcentury[1] ,greatdevelopmentshavebeenob tainedinthetraditionalsulfideslongafterglowluminescentmaterials.Butitspoorchemicalstability ,lowbrightnessandshortafterglowtimecan’tmeettherequirementsofapplica tion .In 1992 ,aluminatessystem[2 ] materialsdopedwithvariousrareearthionswerefoundtohavepropertiesoflongafterglow .Itsafterglowbrightnessisover 10timesofthetra ditionalsulfidesystemmaterials,buttherearesomeshortages…     

长余辉材料余辉性能测试的影响因素

为了规范长余辉材料余辉性能测试的标准化，采用屏幕亮度计测试了SrAl2O4：Eu^2＋，Dy^3＋长余辉材料的余辉性能；研究了激发光源、激发时间、样品粒度和用量对余辉性能测试的影响，结果表明在9W三基色灯下激发15min可使余辉材料发光亮度达到饱和，随着样品粒径增大和质量增加，发光强度明显增强，余辉时间也显著延长．     

长余辉发光材料Zn_2SiO_4:Dy~(3+)的制备及发光性能

以Zn2SiO4为基质，用高温固相法（ss），sol-gel法（sg）制备得到Zn2SiO4：Dy^3＋长余辉发光材料，该发光材料的制备及长余辉发光性能至今尚未见到文献报道．由该发光材料的激发谱发现，其在紫外的235-350nm范围有吸收，其发射光谱表明，在紫光（378nm，393nm）、橙光（595nm）、红光（691nm）部位有发射峰．通过对比掺杂与未掺杂样品发射光谱，说明样品发光是由基质Zn2SiO4产生的，Dy^3＋的掺杂只是使材料形成了陷阱能级进而发出长余辉，还阐述了Zn2SiO4：Dy^3＋的可能发光机理．     

The optical afterglow of the short gamma-ray burst GRB 050709

It has long been known that there are two classes of gamma-ray bursts (GRBs), mainly distinguished by their durations. The breakthrough in our understanding of long-duration GRBs (those lasting more than approximately 2 s), which ultimately linked them with energetic type Ic supernovae, came from the discovery of their long-lived X-ray and optical 'afterglows', when precise and rapid localizations of the sources could finally be obtained. X-ray localizations have recently become available for short (duration <2 s) GRBs, which have evaded optical detection for more than 30 years. Here we report the first discovery of transient optical emission (R-band magnitude approximately 23) associated with a short burst: GRB 050709. The optical afterglow was localized with subarcsecond accuracy, and lies in the outskirts of a blue dwarf galaxy. The optical and X-ray afterglow properties 34 h after the GRB are reminiscent of the afterglows of long GRBs, which are attributable to synchrotron emission from ultrarelativistic ejecta. We did not, however, detect a supernova, as found in most nearby long GRB afterglows, which suggests a different origin for the short GRBs.