首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 906 毫秒
1.
电子回旋脉■和太阳微波毫秒级尖峰辐射   总被引:2,自引:0,他引:2  
本文提出由非热电子(60keV)的空心束(hollow beam)分布激发回旋脉降作为太阳微波毫秒级尖峰辐射的产生机制。文中求得了非常波模二次谐波的增长率及其随时间的变化、脉泽的饱和时间、饱和波能密度及脉降辐射的方向特征。 结果得到,当磁场强度B=507G,等离子体数密度n_(?)=4×10~9cm~(-3),电子温度T_e=1.4×10~6K,非热电子数密度与热电子数密度之比(n_s/n_e)≈4×10~(-5),磁场标高时,将在2.84GHz频率上产生高亮温度(T_b≈5×10~(15)K)的毫秒级尖峰辐射。  相似文献   

2.
俞雪华  徐民健 《天文学报》1995,36(4):359-366
本文采用等离子体动力学方法,研究了日冕条件下磁化非相对论热等离子体对太阳射电辐射产生的电子回旋共振吸收,并在辐射频率等于电子回旋谐波频率时求得n≥2谐波吸收率的近似表示式,以及其对等离子体温度,出射角度和谐波数的变化规律,在应用部分,讨论了电子回旋共振吸收对于太阳射电尖峰爆发的影响,认为目前观测到的尖峰爆,大多数高能电子束来自日冕的内层。  相似文献   

3.
一个太阳耀斑约含数千个微耀斑[1],每个微耀斑以热的,低频波和加速粒子的形式释放能量。耀斑期间大部分能量的释放是通过电子加速转移的结果,然而电子加速是在耀斑前相开始,并在整个耀斑持续期间继续保持。在耀斑发展的不同相期间伴有各种各样的射电辐射现象(及其它波段共生现象),多波段射电观测和比较可以给出有关电子加速过程和耀斑自身发展的重要信息,尤其可检测加速开始的时间和频率部位(目前仍为太阳物理的前沿)。微耀斑能量的瞬时释放可能是引起不同类型快速精细结构的原因,射电毫秒级尖峰辐射是起因于连续能量释放的证据,其辐射源位于或靠近能量释放区[2],公认射电辐射的快速结构是日冕电子束的特征信号[3,4],所以今后使用高时间和高频率分辨率的宽带频谱仪同时观测可详细地探测加速过程,从而对预耀斑的加热和初始能量释放,耀斑的逐步建立和演化都具有重要意义。本文介绍几个典型事件,包括射电尖峰脉冲辐射,类尖峰辐射和短时标漂移结构  相似文献   

4.
谢瑞祥  汪敏 《天文学报》1996,37(2):187-200
作为微耀斑能量释放的证据,本文扼要介绍了云南天文台“四频率太阳射电高时间分辨率同步观测系统”(1.42,2.13,2.84和4.26GHz)1989年12月-1993年4月的观测事例,包含低强度的毫秒尖峰辐射(msspike),类尖峰辐射(spike-like),快速脉动现象,两种新的快速精细结构──微波Ⅲ型爆和微波类斑点结构.统计了快速精细结构的寿命,在统计基础上分别以实例描述了各类现象的观测特征.  相似文献   

5.
一般认为,Langmuir波(LW)转换为电磁波是太阳Ⅲ型射电爆的产生机制。由电子束流不稳定性可以很容易地激发LW,正向LW和反向LW的相互作用被认为是产生Ⅲ型爆二次谐波的原因,但反向LW的色散方程和产生机制尚未得到充分研究。通过粒子(Particle In Cell,PIC)模拟研究了反向LW的产生机制,发现反向LW不能由电子束流直接激发,其能量基本上是由正向LW散射得到的。然而,电子束流对正向LW的二次谐波有直接放大作用。  相似文献   

6.
李明 《天文学报》2011,52(2):93-104
为了研究不同宇宙学模型下弱引力透镜效应的性质,利用N-体模拟产生的数据,通过光线追踪技术,生成二维的κ样本.对应于不同的暗能量状态方程参数的模型,即w=-0.8,w=-1.0,w=-1.2,生成了3组样本.对于这些模型所生成的样本视场均为3°×3°,并假设所有作为背景源的星系都分布在z=1处的平面上.对这些κ场的样本均进行了尖峰统计和尺度-尺度相关的统计.对尖峰的统计结果显示,包含噪声的κ场中尖峰分布在不同模型下的差别还是存在的.噪声改变了中等幅值和小幅值的尖峰分布,而对高幅值的尖峰分布影响不大.同时降噪后κ场中高幅值尖峰分布的结果表明,降噪后不同模型间高幅值尖峰分布的差别还是非常明显的.对于尺度-尺度相关统计,分析了不同模型的尺度-尺度相关系数的累积概率分布函数,w=-1.2的模型与w=-0.8和w=-1.0的模型的差别能达到20%和30%.因此尺度-尺度相关的统计结合尖峰数目的统计,可以做为确定暗能量状态参数的一种新的手段.  相似文献   

7.
根据不同的发射波模以及偏振态(偏振度与偏振方向)的快速时变特征,对1993年10月2日07:44:34-07:44:52:99UT期间的太阳射电事件进行了证认,认为这是一个由两群、总数约为40个尖峰(spike)结构组成的罕见的宽带事件,它的总带宽>300MHz、相对带宽■5%.根据它们在2.545GHZ,2.645GHZ;2.695GHZ和2B40GHZ上的流量资料,首次对一些spike结构作了谱分析.发现spike结构谱的峰值频率,第一群呈现为随时间由高频向低频漂移的倾向,第二群基本上位于2.695GHZ上.Spike谱的这些观测特征,可定性地用非热电子束流平均能量的时变特性来解释.对于第二群具有相同峰值频率的spike辐射,可能来自同一电子回旋脉泽不稳定区域.  相似文献   

8.
马春玉  黄光力 《天文学报》1995,36(3):309-313
本文作者用相对论电子束在等离子体中运动时的色散关系讨论了纵向传播的波模的稳定性,发现静电Langmuir波和Alfven波是不稳定的,并计算了其增长率,而高频电磁模和硝声模是稳定的。相对论电子束激发的Langmuir波和Alfven波的不稳定性可用于解释射电喷流中相间的热斑、粒子再加速、辐射机制以及能量传输问题。  相似文献   

9.
太阳Ⅲ型暴与反向Langmuir波的产生   总被引:1,自引:0,他引:1  
黄宇  黄光力 《天文学报》2007,48(4):441-448
一般认为,Langmuir波(LW)转换为电磁波是太阳Ⅲ型射电暴的产生机制.由电子束流不稳定性可以很容易地激发LW,正向LW和反向LW的相互作用被认为是产生Ⅲ型暴二次谐波的原因,但反向LW的色散方程和产生机制尚未得到充分研究.对含有温度的双流不稳定性的方程进行了解析求解,发现温度和束流速度分别对反向和正向LW色散关系具有显著影响,并采用粒子模拟(PIC)方法部分证实了解析推导的结果.通过PIC模拟研究了反向LW的产生机制,发现反向LW不能由电子束流直接激发,其能量基本上都是由正向LW散射得到的.然而,电子束流对正向LW的二次谐波有直接放大作用.  相似文献   

10.
向梁  吴德金  陈玲 《天文学报》2023,64(3):27-77
动力学阿尔文波是垂直波长接近离子回旋半径或者电子惯性长度的色散阿尔文波.由于波的尺度接近粒子的动力学尺度,动力学阿尔文波在太阳和空间等离子体加热、加速等能化现象中起重要作用.因此,动力学阿尔文波通常被认为是日冕加热的候选者.本研究工作深入、系统地调研了太阳大气中动力学阿尔文波的激发和耗散机制.基于日冕等离子体环境,介绍了几种常见的动力学阿尔文波激发机制:温度各向异性不稳定性、场向电流不稳定性、电子束流不稳定性、密度非均匀不稳定性以及共振模式转换.还介绍了太阳大气中动力学阿尔文波的耗散机制,并讨论了这些耗散机制对黑子加热、冕环加热以及冕羽加热的影响.不仅为认识太阳大气中动力学阿尔文波的驱动机制、动力学演化特征以及波粒相互作用提供合理的理论依据,而且有助于揭示日冕等离子体中能量储存和释放、粒子加热等能化现象的微观物理机制.  相似文献   

11.
本文简要回顾了太阳射电米波爆发中尖峰事件的研究现状。对与之相关的一些内容作了介绍,同时,我们也提出了研究设想和展望  相似文献   

12.
De-Yu Wang  Ding-Yi Li 《Solar physics》1991,135(2):393-405
A model of nonlinear parametric instability (NLPI) modulation is suggested to explain the millisecond spikes in solar decimetric radio emission. The radio emission energy will periodically transfer to two other waves, and the intensity of the radio emission will be modified by NLPI processes in the corona, when the matching conditions of three-wave coupling are satisfied. This model can simultaneously explain the duration of spikes, why the millisecond spikes have not been observed in other solar radio emission, and the relation between the duration of the spikes and the intensity and the frequency of the radio emission as well.  相似文献   

13.
The multibeam propagation of radio waves in the solar plasma is analyzed, because the emission from a solar flare passes through an inhomogeneous solar atmosphere on its way to the observer. A formula (a mathematical model) for calculating the structure of the dynamic spectrum for flare radio bursts has been obtained. Comparison of the calculated spectra with the observed ones shows that the results of interference explain the formation of a zebra structure and the separation of its stripes into individual spikes, describe the time profile of the spikes, and explain the properties of fibers, ropes of fibers, and chains of “point” bursts. The similarity of the dynamic spectra testifies that the fine structure of the spectra is formed not in the emission source but as a result of the propagation of waves through the solar corona and interplanetary space.  相似文献   

14.
A theoretical analysis of electron-cyclotron maser instabilities indicates that the distribution function of non-thermal electrons influences millisecond radio spikes in solar flares, and that a hollow beam distribution is more likely than a loss-cone distribution. The restrictions of classical theories of cyclotron resonant absorption are discussed and a formula is derived for the absorption coefficient near the resonant frequency. Finally, the computations show that for typical coronal parameters, the growth rates of the fundamental of fast extraordinary modes are much faster than those of their second harmonics; and because the directional angle of the fundamental is smaller, its resonant absorption may be neglected. Moreover, the band-width of the fundamental is consistent with observation of radio spikes; therefore, we claim that the millisecond radio spikes in the decimetric range are composed mainly of fundamentals of the fast extraordinary modes. The second harmonics of fast extraordinary modes may be generated for directions near to the vertical to the magnetic field, but it is impossible to observe both fundamental and second harmonics in the same direction.  相似文献   

15.
Radio observation is one of important methods in solar physics and space science. Sometimes, it is almost the sole approach to observe the physical processes such as the acceleration, emission, and propagation of non-thermal energetic particles, etc. So far, more than 100 solar radio telescopes have been built in the world, including solar radiometers, dynamic spectrometers, and radioheliographs. Some of them have been closed after the fulfillment of their primary scientific objectives, or for their malfunctions, and thus replaced by other advanced instruments. At the same time, based on some new technologies and scientific ideas, various kinds of new and much more complicated solar radio telescopes are being constructed by solar radio astronomers and space scientists, such as the American E-OVSA and the solar radio observing system under the framework of Chinese Meridian Project II, etc. When we plan to develop a new solar radio telescope, it is crucial to design the most suitable technical parameters, e.g., the observing frequency range and bandwidth, temporal resolution, frequency resolution, spatial resolution, polarization degree, and dynamic range. Then, how do we select a rational set of these parameters? The long-term observation and study revealed that a large strong solar radio burst is frequently composed of a series of small bursts with different time scales. Among them, the radio spike burst is the smallest one with the shortest lifetime, the narrowest bandwidth, and the smallest source region. Solar radio spikes are considered to be related to a single magnetic energy release process, and can be regarded as an elementary burst in solar flares. It is a basic requirement for the new solar radio telescope to observe and discriminate these solar radio spike bursts, even though the temporal and spatial scales of radio spike bursts actually vary with the observing frequency. This paper presents the scaling laws of the lifetime and bandwidth of solar radio spike bursts with respect to the observing frequency, which provide some constraints for the new solar radio telescopes, and help us to select the rational telescope parameters. Besides, we propose a spectrum-image combination mode as the best observation mode for the next-generation solar radio telescopes with high temporal, spectral, and spatial resolutions, which may have an important significance for revealing the physical essence of the various non-thermal processes in violent solar eruptions.  相似文献   

16.
Solar radio spikes are one of the most intriguing spectral types of radio bursts. Their very short lifetimes, small source size and super-high brightness temperature indicate that they should be involved in some strong energy release, particle acceleration and coherent emission processes closely related to solar flares. In particular, for the microwave spike bursts, their source regions are much close to the related flaring source region which may provide the fundamental information of the flaring process. In this work,we identify more than 600 millisecond microwave spikes which recorded by the Solar Broadband Radio Spectrometer in Huairou(SBRS/Huairou) during an X3.4 solar flare on 2006 December 13 and present a statistical analysis about their parametric evolution characteristic. We find that the spikes have nearly the same probability of positive and negative frequency drifting rates not only in the flare rising phase, but also in the peak and decay phases. So we suppose that the microwave spike bursts should be generated by shockaccelerated energetic electrons, just like the terminational shock(TS) wave produced by the reconnection outflows near the loop top. The spike bursts occurred around the peak phase have the highest central frequency and obviously weak emission intensity, which imply that their source region should have the lowest position with higher plasma density due to the weakened magnetic reconnection and the relaxation of TS during the peak phase. The right-handed polarization of the most spike bursts may be due to the TS lying on the top region of some very asymmetrical flare loops.  相似文献   

17.
As evidence for energy release in microflares, high time resolution observations of solar radio emission obtained with our “synchronous observation system of solar radio radiation with high time resolution at four frequencies (1.42, 2.13, 2.84 and 4.26 GHz)” from December 1989 to April 1993 are presented in this paper. The observed events include weak ms spikes, “spike-likes”, fast pulsations as well as two kinds of newly discovered fast fine structures, i.e., microwave type III bursts and microwave patch-like structures. A statistical study of the duration of fast fine structures has been made and on its basis the various types of phenomena are illustrated with actual examples.  相似文献   

18.
Hong-Wei Li 《Solar physics》1987,111(1):167-173
In this paper the evolution of the hollow beam distribution of energetic electrons giving rise to ECM instability is investigated and the spatial dispersion term is included in the equation of wave energy. The instability causes the growth of wave energy, while the propagation of waves evacuates the electromagnetic energy from the source region. By analysing these two effects spike-like time profiles of waves are obtained. It is found that the saturation time t s of ECM emission and the duration of spikes increase with the decrease of the frequency of solar radio spike emission. The approximate expressions of t sand of the peak wave energy density are derived.Proceedings of the Second CESRA Workshop on Particle Acceleration and Trapping in Solar Flares, held at Aubigny-sur-Nère (France), 23–26 June, 1986.On leave from the Department of Astronomy, Nanjing University, Nanjing, People's Republic of China.  相似文献   

19.
丁祖高 《天文学报》1998,39(3):324-332
对自适应矢量量化(SAVQ)技术在太阳射电频谱数据压缩中的应用进行了有意义的讨论.给出一种压缩比和失真可调的SAVQ压缩方法,指出提高数据压缩比的有效方法之一为样本集成,同时介绍了用该技术对北京天文台太阳射电频谱仪上的两个波段(1.0GHz-2.0GHz和2.6GHz-3.8GHz)的观测数据进行压缩的实用效果,并与国际同行所用的ICON方式进行性能比较.最后展示了数据压缩技术及其在天文上的应用.  相似文献   

20.
利用北京天文台 2.6—3.8 GHz频谱仪的观测资料,找到 11个微波尖峰辐射事件.尖峰一般具有数十毫秒的寿命,数百个sfu的流量密度和数十至数百MHz的带宽,这与以前的报道类似.尖峰的偏振度各式各样,有的尖峰还有数千MHz/s的频率漂移.某些尖峰在二个偏振态之间有8毫秒的时间延迟(最大延迟可达16毫秒).另外,还发现了尖峰的偏振度随频率剧烈变化的偏振反转现象.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号