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1.
本文介绍用“三波段太阳射电高时间分辨率同步观测系统”所观测到的1988年12月16日三波段(1420MHz、2840MHz、4000MHz)太阳射电大爆发中毫秒级精细结构的观测特征,指出太阳射电快速活动在射电爆发的不同阶段具有不同的特征,首先在爆发的上升沿出现2840MHz的毫秒尖峰辐射群,继而在1420MHz上出现毫秒级尖峰辐射群,并且还在以后的几个爆发次峰上陆续出现,在长达两小时的大爆发过程中,在4000MHz上始终未产生毫秒级尖峰辐射,这也反应了射电尖峰辐射现象存在着一定的带宽。特别引起注意的是毫秒级尖峰辐射群均出现在射电爆发的峰值附近,在其它时间的记录中尚未发现毫秒尖峰辐射。 三波段的秒级射电爆发曲线如图1所示。毫秒级精细结构如图2所示。由图2可见,单个尖峰辐射的持续随频率的减小而增加,2840MHz多为10—20ms,1420MHz多为30—170ms;所产生的尖峰辐射群强度不大,而且很少有孤立的尖峰;2840MHz尖峰辐射的强度一般为450—900sfu,1420MHz一般为500—1770sfu(1sfu=10~(-22)WM~(-2)Hz~(-1));还特别引起注意的是在2840MHz上当所出现的尖峰辐射群结束时,往往出现持续时间为100ms的流量下降现象,(此种现象在以往的观测中未曾见过),详见图2b和2c;关于事件尖峰辐射的丰度,仅对几个尖峰辐射群作了统计如下: 在1420M  相似文献   

2.
Boulder美国空间环境服务中心(SESC)发布245MHz射电爆发资料作为太阳活动实时警报。本文介绍这个频段射电爆发的特点、观测情况并结合云南天文台的米波射电频谱观测资料讨论这个频段的窄带射电爆发与其他太阳活动的关系。  相似文献   

3.
分析了国家天文台云南天文台射电频谱仪在230~300MHz、625~1500MHz、1000~2000MHz和2600~3800MHz记录到的11对具有双向漂移结构的Ⅲ型爆发.对双向Ⅲ型爆发的半功率持续时间、频率漂移率、偏振度等观测特征与普通Ⅲ型爆发作了比较,与Hα耀斑的关系也作了详细分析.得到这些事件的显著特征,并对双向Ⅲ型爆发作了定性解释.  相似文献   

4.
综述云南天文台在太阳活动22周峰年期间观测到的米波射电频谱资料,处理资料时发现230~300MHz频段有一些有趣的观测现象。如米波Ⅲ型爆发;“blips”;毫秒级Spike与Ⅲ型爆发共存事件;快速脉动等。根据这些事件的现象,讨论了它们的产生机制。  相似文献   

5.
本文分析了2002.7.23国家天文台云南天文台射电频谱仪在625~1500 MHz、2600~3800 MHz和5200~7600 MHz记录到的复杂型大爆发,将此爆发与Hα耀斑、日冕物质抛射(CME)、硬X射线爆发及地球物理参数作了相关分析,得到这个事件的一些显著特征,认为这一事件电子的加速区在日冕的外层,接近625 MHz的地方,并且多次发生磁重联.磁重联以后的衰变相是湍流加速过程.  相似文献   

6.
北京天文台1 .02 .0GHz 太阳射电频谱仪从1994 年开始观测至1998 年9 月记录到太阳射电爆发171 个,2 .63 .8GHz 太阳射电频谱仪1996 年9 月投入观测至1998 年9 月,记录到146 个太阳射电爆发。1998 年4 月15 日太阳射电爆发同时在这两台频谱仪上记录到。这个事件在时间和频率上显示了丰富的幅度和结构的变化。发现了微波Ⅲ型爆发对群,并存在着丰富的快速活动现象。取得了高时间分辨率、高质量的动态谱资料,为研究耀斑各种尺度的时间及空间演化过程提供了丰富的信息。  相似文献   

7.
利用国家天文台云南天文台“分米波(700—1500MHz)射电频谱仪”和“四波段太阳射电高时间分辨率同步观测系统”分别于2001年6月24日和1990年7月30日观测到了两个稀少事件,前者是一个小射电爆发,其上升相伴随有短周期(约29、40和100毫秒)的脉动,后者是一个射电大爆发,在2840MHz上产生了周期约30毫秒的射电脉动,还着重讨论其甚短周期(如29—40毫秒)的脉动现象,甚短周期脉动可能是归因于起源在日冕深处不稳定区域的哨声波束周期链对射电辐射的调制,或沉降电子束驱动的静电高混杂波,经由波-波非线性相互作用导致甚短周期的射电脉动。  相似文献   

8.
太阳射电爆发是无线通讯特别是卫星导航通讯的潜在影响因素之一.2015年11月4日的太阳射电爆发事件在1415 MHz点频的流量达到了峰值5800 SFU(Solar Flux Unit,太阳射电流量单位,1 SFU=10-22 W/(m2·Hz)),位于日下点的欧洲全球定位系统(Global Positioning S...  相似文献   

9.
为完成对太阳射电爆发15 MHz~15 GHz频谱的监测,云南天文台研发4套太阳射电频谱仪,频率覆盖范围依次为15~80 MHz, 100~750 MHz, 600~4 200 MHz和4~15 GHz,分别称为十米波、米波、分米波和厘米波太阳射电频谱仪。十米波段太阳射电频谱仪的谱分辨率和时间分辨率分别为7.6 kHz和1 ms;米波段和分米波段太阳射电频谱仪的谱分辨率和时间分辨率分别为9.5 kHz和10 ms;厘米波段太阳射电频谱仪的谱分辨率和时间分辨率分别为76 kHz和10 ms。每套设备包括天线系统、接收机和数字频谱仪。为实现超高谱分辨率,需要的快速傅里叶变换(Fast Fourier Transform, FFT)点数最高达到262 144,在现场可编程门阵列(Field Programmable Gate Array, FPGA)上,通过一个FFT IP核(Intellectual Property Core)不能实现如此高点数的快速傅里叶变换运算。对于大点数的快速傅里叶变换,需要对数据行列分解后做并行处理,从而将其转化为两个小点数的快速傅里叶变换。通过对并行算法的研究,...  相似文献   

10.
利用云南天文台声光频谱议1991年6月观测到的来自6659活动区的米波射电爆发记录,及其光学活动、磁场速度场的资料,作了分析研究。得到了一些有意义的结果  相似文献   

11.
用云南天文台高时间分辨率(10ms)高频率分辨率(0.5MHz)的射电频谱仪观测分析证认了米波窄带短持续时间快频漂爆发的存在.这种爆发既不同于经典的III型爆发,也不同于spike和I型爆发,是一种新的米波爆发型别.它的特性与分米波的“blips”相近.  相似文献   

12.
Using the decimetric (700–1500 MHz) radio spectrometer and the synchronous observational system with high temporal resolution at four frequencies (1420, 2130, 2840 and 4260 MHz) of Yunnan Observatory, two rare events were observed on 2001 June 24 and 1990 July 30. The former was a small radio burst exhibiting pulsations with short periods (about 29, 40 and 100 ms) in the impulsive phase. The latter was a large radio burst, which at 2840 MHz produced radio pulsations with period of about 30 ms. This paper focuses on pulsations with very short periods in the range of 29–40 ms. The mechanism of generation of such pulsations may be modulation of radio radiation by the periodic trains of whistler packets originating in unstable regions of the corona. Alternatively, these pulsations can be attributed to wave-wave non-linear interactions of electrostatic upper hybrid waves driven by beams of precipitating electrons in flaring loops.  相似文献   

13.
Ourmeterwavesolarradioacousto -opticalspectrograph(AOS)tracesbacktotheyear 1 979whenitwasbeingbuilt.TheAOScoversaworkingfrequencyrangeof 2 30~ 30 0MHz .Ithasthemeritsofhighspectralresolutionandgoodsensitivity .Thespectralresolution( 0 2 5MHz)de pendsonthecharacteris…  相似文献   

14.
太阳米波和分米波的射电观测是对太阳爆发过程中耀斑和日冕物质抛射现象研究的重要观测手段。米波和分米波的太阳射电暴以相干等离子体辐射为主导,表现出在时域和频域的多样性和复杂性。其中Ⅱ型射电暴是激波在日冕中运动引起电磁波辐射的结果。在Ⅱ型射电暴方面,首先对米波Ⅱ型射电暴的激波起源问题和米波Ⅱ型射电暴与行星际Ⅱ型射电暴的关系问题进行了讨论;其次,结合Lin-Forbes太阳爆发理论模型对Ⅱ型射电暴的开始时间和起始频率进行讨论:最后,对Ⅱ型射电暴信号中包含的两种射电精细结构,Herringbone结构(即鱼骨结构)和与激波相关的Ⅲ型射电暴也分别进行了讨论。Ⅲ型射电暴是高能电子束在日冕中运动产生电磁波辐射的结果。在Ⅲ型射电暴方面,首先介绍了利用Ⅲ型射电暴对日冕磁场位形和等离子体密度进行研究的具体方法;其次,对利用Ⅲ型射电暴测量日冕温度的最新理论进行介绍;最后,对Ⅲ型射电暴和Ⅱ型射电暴的时间关系、Ⅲ型射电暴和粒子加速以及Ⅲ型射电暴信号中包含的射电精细结构(例如斑马纹、纤维爆发及尖峰辐射)等问题进行讨论并介绍有关的最新研究进展。  相似文献   

15.
在1990年7月30日观测到的太阳射电大爆发中,在1420MHz和2000MHz两个波段上发现了长周期(数+秒)的脉冲现象。经数据处理分析,发现了几个特点:(1)脉冲的宽带大于600MHz。(2)1420MHz上的脉动的周期较2000MHz上脉动的周期大,相对强度也是前者较大。(3)脉冲的相对强度随脉冲周期的增大而增大,呈较好的线性关系  相似文献   

16.
The 13 pairs of type III bursts with the bidirectional drift structures recorded with the spectrograph in the frequency ranges of 230–300 MHz and 625–1500 MHz at the Yunnan Observatory and 2600–3800 MHz at the Beijing National Astronomical Observatories are analyzed in this present article and the outstanding characteristics of these events are obtained. These bursts respectively reveal that the separatrix frequency between the bursts with positive and negative drifts comes between 250 MHz and 3420 MHz, with a gap being between 0.6 MHz and 110 MHz; the duration is 53 ms–1880 ms and the frequency drift rate is between 45 MHz/s and 56000 MHz/s. The drift rate at metric wavelengths is relatively low, only a few decades of MHz while it is comparatively high at microwave wavelengths, reaching 56000 MHz/s. The qualitative explanation of these events is given in this paper.  相似文献   

17.
The solar burst event of 1992-06-07 is analyzed in this paper using HXR material of the Yohkoh satellite and radio data at 2840 MHz observed at Beijing Astronomical Observatory. The results show that during the impulsive phase, the pulsational component had two time scales, a longer one of about 30 s, and a shorter one of 1–4 s. The pulsations on the longer scale are found to be correlated with a series of variations in the HXR images of the source region. A physical picture comprising loop-loop interaction and MHD oscillation modulation is presented.  相似文献   

18.
Ya. G. Tsybko 《Solar physics》1984,92(1-2):299-315
Type-IIIb, IIId, and III solar decametric radio bursts, being distinguished by the typical negative drift rate of their dynamic spectra, are compared. Observational data were obtained with a UTR-2 antenna during the period 1973–1982. During the analysis of the bursts of all these spectral varieties, the frequency drift time (drift delay) was measured in the ranges 25 to 12.5 MHz, 25 to 20 MHz, and 12.5 to 10 MHz. Durations of type-III bursts were determined at the harmonically-related frequencies of 25 and 12.5 MHz; radio source locations were also used.It is shown that these decametric bursts are distinctly divided into two groups: (1)type-IIIb chains of simple stria bursts and also normal type-III storm bursts observed at central regions constitute a group of events with a fast drifting spectrum; (2) type-III bursts from type-IIIb-III pairs and the limb variant of normal III bursts, as well as peculiar type-IIId chains of diffuse striae and related chains with an echo component, constitute a second group of events with comparatively slow drift rates.The first group of the phenomena is associated with the fundamental F frequency and the second one, with the harmonic H of the coronal plasma frequency. The results of the present investigation agree well with earlier conclusions on the harmonic origin of decametric chains and type-III bursts. Measurements of drift delays in narrow frequency ranges, an octave apart, as well as type-III burst durations at harmonically-related frequencies confirm the existence of both F and H components in the solar radiation. The essential result of 10 years of decametric observations is that the frequency drift rates and durations are rather stable parameters for the various type-III bursts and stria-burst chains. The stability characterizes some unspecified conditions of burst generation in the middle corona.  相似文献   

19.
本文研究了寻常波和非常波在线性传播条件下,对快速毫秒级spike的时延、频漂和偏振逆转的影响.计算表明,在(20-40)×Baumbach-Alien的电子密度分布下,由于传播产生的时延,偏振逆转等约为30-300ms,这与观测结果在量级上是一致的.这说明在快速活动中传播效应是一个重要的因素.  相似文献   

20.
From radio spectra between 160 and 320 MHz of chains of type I bursts it appears that their duration distributions allow an exponential fit, and that those of samples containing long and short chains respectively, taken from the same storm, have virtually the same characteristic time (logarithmic slope). On the average this figure decreases - as a function of the frequency - at about 1 s per 10 MHz. The high frequency cut-off of chain activity (noise storms) is mainly a consequence of the frequency dependence of the probability for the first burst of a chain to appear. Given the density of type I bursts in a chain, it is concluded that the probability of a type I burst to be followed by another one is at least 90% below 250 MHz and 70–80% at 300 MHz, which makes it essential for type I theories to include a mechanism to this effect. The drift rate distribution for chains is symmetrical with a peak at-10 MHz/s. The statistics is indicative of a correlation between drift rate and duration. No evidence has been found for the occurrence of chain pairs or frequency splitting in chains, nor for an association between chains and type III bursts.  相似文献   

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