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1.
对澳大利亚Culgoora天文台射电频谱仪在太阳活动第23周峰年期间记录到的米波Ⅲ型爆发(20~420 MHz),与日冕物质抛射(CME)、Hα耀斑及相关事件进行了统计分析,发现米波Ⅲ型爆发与CME的关系没有Ⅱ、Ⅳ型爆发与CME的关系密切;米波Ⅲ型爆发发生的时间在CME之前25~30 min最多;72%的CME事件伴随长寿命的Hα耀斑.从这些观测特征出发,对米波Ⅲ型爆发、CME和Hα耀斑进行了定性的解释.   相似文献   

2.
本文对1989年4月9日与4B级大耀斑伴生的两个波段(3750 MHz,2840 MHz)的射电大爆发进行了简单的初步分析。结果表明:这两个波段的爆发不仅各自具有繁多的周期,而且都存在30+3s的准周期振荡。这种现象可能与磁环的准周期振荡有关,或与粒子流有关。   相似文献   

3.
本文根据1981年HALE 17590 太阳活动区的观测资料,着重分析了它的射电辐射特性后发现:(1)在光学活动区发展的上升阶段,每串射电爆发的强度也有由弱到强的变化,其频谱由单调谱变成不规则谱和U型谱;(2)对大的耀斑爆发而言,射电爆发的先兆相比X射线爆早。在射电先兆相期间常伴有谱斑增亮和暗条激活等现象;(3)大耀斑爆发的脉冲极大时刻在射电8毫米波段到来最早。   相似文献   

4.
通过分析"云南天文台4波段太阳射电快速同步观测系统"1990-01-1994-01取得的103个射电爆发,发现其中29个存在不同类型的快速精细结构(FFS).尤其是发现了几个少见的亚类FFS现象.本文仅介绍两个亚类型:窄带变周期脉动和宽带慢漂移长周期脉动.这些现象表明太阳射电FFS的多样性,它们发生在射电爆发的不同阶段(耀斑不同相),从而说明在耀斑演化中日冕非热电子的加速或注入可能贯穿于整个耀斑发展过程.由于耀斑后相FFS的发生,可验证耀斑后相存在磁重联和似环结构(耀斑后环)的重新形成.由于不同的亚类FFS反映日冕中存奇特别的环境条件,从而推测日冕中可能存在更复杂的多重类型的磁结构.   相似文献   

5.
本文比较第17—21太阳周黑子数、地磁A_p指数、各周极大年≥2级耀斑数、磁暴数及第一、二、三大磁暴情况;分析了≥2级耀斑数及磁暴的分布。21周3级耀斑对应磁暴比例低于19、20周,Ⅳ型及米波射电爆发是产生磁暴的重要条件。进一步分析了21周最大磁暴、最大射电爆发引起的磁暴,最严重的电离层短波通讯干扰及有明亮物质抛射的大耀斑、双带大耀斑引起的磁暴等典型例子。最后对SMY期间22个无黑子耀斑作了分析,它们可能引起中小幅度的磁暴。   相似文献   

6.
太阳微波爆发动态频谱仪   总被引:2,自引:1,他引:1  
介绍了北京天文台已投入观测的1.0—20GHz,2.6—3.8GHz太阳射电频谱仪及1999年投入观测的5.2—76GHz太阳射电频谱仪。它们是第23周太阳活动峰年我国太阳物理界的重要观测设备已投入观测的频谱仪获得不同类型的太阳射电爆发资料分别为171个和146个,这些事件在时间和频率上有丰富的幅度和结构的变化。不同太阳射电爆发反映太阳大气不同高度上耀斑的时间和空间的演化过程,为研究不同大气高度中耀斑物理动力学过程、能量释放、粒子加速提供了更多的依据。   相似文献   

7.
利用光学、射电、软X射线和硬X射线观测资料,对1986年2月系列太阳爆发中最大的两个耀斑作相似与相异性的分析,解释它们近地空间效应的区别,对该系列太阳爆发事件和叠加在一起的地球事件作认证研究。  相似文献   

8.
利用光学、射电、软X射线和硬X射线观测资料,对1986年2月系列太阳爆发中最大的两个耀斑作相似与相异性的分析,解释它们近地空间效应的区别,对该系列太阳爆发事件和叠加在一起的地球事件作认证研究.   相似文献   

9.
统计分析了太阳第23周期间(2000年7月至2004年9月)在625~1500,MHz,2600~3800,MHz和5200~7600,MHz范围频谱仪观测到的Ⅲ型射电爆发. 给出了Ⅲ型爆发的分布、寿命、频率漂移率、偏振度和频率带宽. 结果显示, 频率漂移率和频率带宽的平均值随频率的增加而增大, 寿命和偏振度的平均值既不是常数也不是在宽频延伸上保持均匀不变的.最多的Ⅲ型爆发分布在625~3800,MHz范围内, 且随频率的增加而增多. 分析表明, 电子加速和能量释放地点主要是在分米波范围内, 这个频率范围的特征可能与分米波段上的磁位形有关, 并且与主耀斑地点附近磁重联区中的电子加速有关. 然而, 还有相当数量的Ⅲ型爆发发生在5200~7600,MHz范围内, 这个特征表明电子加速的地点是在一个日冕的宽范围中. 关于厘米relax-relax 分米波段Ⅲ型爆发的辐射机制最可能包含相干的等离子体辐射或电子回旋脉泽辐射过程.   相似文献   

10.
AR5395和AR5629X射线事件的太阳射电辐射特征吴洪敖,孙九祯(中同科学院紫金山天文台,南京210008)关键词太阳耀斑,X射线事件,射电事件一、概况本文选用的典型事件是1989年3月的AR5395和8月的AR5629的射电缓变和爆发分量,及其...  相似文献   

11.
High correlation between microwave bursts and Hα flares has already been reported. However, Solar Maximum Year cooperation made it possible to do simultaneous observations of selected active regions with good spatial resolution. In this paper the results of the direct comparison of solar microwave recordings at the Metsähovi Radio Research Station and Hα films at the Hvar Observatory are reported. This comparison reveals that the correlation of microwave gradual rise and fall (GRF) events (time scale tens of minutes) with Hα flares is practically 100 percent. On the other hand the correlation of the impulsive microwave bursts (time scale tens of seconds) with Hα flares is low. From this it can be concluded that the main contribution to the microwave GRF bursts comes from thermal radiation.  相似文献   

12.
北京天文台在2.84GHz频率上观测到的带短时标精细结构的微波爆发与日本YOHKOH卫星上HXT在1991年10月-1992年12月观测到的硬X射线爆发(HXB)事件作了比较,发现在20个微波精细结构爆发事件只有12个与YOHKOH卫星记录的HXB有对应关系.本文对1992年6月7日典型事件中2.84GHz与HXB共同存在的百秒量级的准周期振荡作了分析及源区参数的计算,并作了简要的讨论.  相似文献   

13.
We present an analysis of five microflares, three observed simultaneously by RHESSI in hard X-rays and Nobeyama RadioHeliograph (NoRH) in microwaves (17 GHz) and two observed by RHESSI and Nancay RadioHeliograph (NRH) at metric wavelengths (150–450 MHz). Since we have no radio imaging telescopes simultaneously operating at microwave and meter wavelengths in the same time zone, we are obliged to use a different set of metric events in contrast to that used for comparison with the two radio wavelengths. We are interested in using the locations and other imaging characteristics of the events from both RHESSI and radio observations instead of just temporal correlation. So we have used the Nancay (France) metric radioheliograph at 150–450 MHz for this purpose. Here we describe the properties of five events – three in microwaves and two at metric wavelengths. We discuss the brightness temperatures, emission measures and the hard X-ray spectral properties of these microevents. One sees small (mini) flaring loops clearly in NoRH and RHESSI images. The microwave emission often seems to come from the RHESSI foot points (for higher energies), and from the entire small (mini) flaring loop (for lower energies).The RHESSI microflares seem to be associated in position with metric type III bursts. Frequently, the hard X-ray spectrum of the microwave associated RHESSI microflares can be fit by a thermal component at low energies (∼3–12 keV) and a nonthermal component at higher energies (∼12–20 keV).  相似文献   

14.
CME在产生和发展过程中与日冕和行星际介质相互作用并发出不同波长的射电辐射.在研究了无CME时空间等离子体的各种辐射机制基础上,统计分析了1999年2月至1999年8月期间有较大的CME发生情况下,在CME影响下L1拉格朗日点附近等离子体参数发生变化后的射电辐射机制.分析结果表明,其射电辐射机制主要是轫致辐射、微量的回旋辐射和更加微弱的复合辐射.此外,分析讨论了1999年2月至1999年8月期间与CME共生的太阳微波爆发.分析结果表明,与CME共生的是微波逐渐型爆发、尖峰爆发,其辐射机制主要是轫致辐射、回旋共振辐射、等离子体辐射及电子回旋脉泽辐射.  相似文献   

15.
Type-III bursts are signatures of the electron beams accelerated during the solar flares, their observation and investigation provide information of the acceleration processes, the characteristics of the exciting agent and the acceleration site. The Brazilian Solar Spectroscope (BSS), in operation at INPE, Brazil, have recorded type-III radio bursts in decimetric range (2050–2250 MHz) with high time resolution of 20 ms. Decimetric reverse drift bursts are possibly generated in a dense loop by electron beams travelling towards the photosphere. Hence their time profiles should carry signatures of the density inhomogenities in the loop. Here the temporal and spectral characteristics of decimetric type-III bursts are presented.  相似文献   

16.
We report high resolution observations of the Intermediate Drift (IMD) bursts in decimetric band (ν = 950 – 2650 MHz). With a time resolution of 20 – 50 ms and a frequency resolution of 4 – 10 MHz, we are able to estimate the characteristics of IMD bursts such as the bandwidth and duration of the emission. Frequency drift rate and its dependence on the frequency are derived for individual IMD structures. All IMD bursts analyzed show negative drift rate. The values are of the order of −28 – −274 MHz s−1. The drift rates normalized by the mean frequency are ranged between −0.20 s−1 and −0.02 s−1. Both the frequency drift rate and its frequency dependence provide important clues to the emission mechanisms of IMD. A comparison and a critique of the existing models based on the plasma and the maser emissions with modulation by Alfvén solitons as well as the whistler wave model are presented.  相似文献   

17.
Due to the lack of simultaneous high sensitivity/time resolution observations at mm- cm-λ and m-λ a program on such investigations has been carried out with data obtained by INPE at Itapetinga and by the Astronomical Observatory of Trieste. Preliminary results obtained by comparing mm-wave burst structures with 408, 327 and 237 MHz indicate that i) for majority of major time structures (time scales of the order of 1 sec) observed at 22 GHz bursts, corresponding type III bursts have been observed at 237 MHz, however ii) start times at mm-λ and m-λ are not often coincident at two wavelengths. These observations favour the hypothesis of (a) time dependent acceleration of energetic electrons and (b) burst emission is the response to a multiple injection of energetic electrons.  相似文献   

18.
With a high time resolution of 1 millisecond, we have observed some ultra-fast fine structures of the microwave bursts at the frequency of 2.84 GHz. A preliminary analysis has shown that the background continuum of the microwave bursts can be interpreted as gyro-synchrotron radiation in large regions while the fast spikes superimposed on the continuum may be generated by plasma radiation in much smaller regions.  相似文献   

19.
Source length scales are estimated for the September 14, 2005 solar noise storm from the spectral and temporal observed characteristics of the background continuum fluctuations and clusters of Type I bursts. The characteristic height of the magnetic structure where the noise storm source is located and the size of the source where Type I bursts clustering takes place were calculated. A lower limit for the height of the magnetic structure supporting the noise storm at 237 MHz was estimated too.  相似文献   

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