太阳X射线爆发与低电离层突然骚扰

本文分析了1981年1月至5月期间记录的低电离层突然骚扰(SID)和太阳X射线爆发数据发现:1.几乎所有的研究情况,每一个低电离层的突然骚扰都是太阳X射线爆发引起的。且SID与太阳X射线爆发之间有着相同的开始和极值时间;2.能够引起低电离层产生较明显的SID的太阳X射线爆发的峰值流量下限对于0.5～4A频段是约4×10~(-3)w/m~2,对1～8A频段是2×10~(-6)w/m~2;3.相关分析表明,太阳X射线爆发的流量变化量与低频记录的突然相位异常(SPA)的变化量之间有好的相关性。根据这个初步的研究有可能利用低频SPA的监测来较好地检测太阳X射线爆发。     

低频甚低频传播突然扰动

SPA甘匆(脾)邹(娜)一2 .9一3 .0一0 .7一0.7一0 .9一1 .7 SPA们T娜(钾) SFA甘△A(dB) 1 .3 ~1 .7 1 .3绷IMPI 卜l教咖(UT)︸05n哪2(X场年6月日开始红Am.弓口.、甘气︸d.几11，1低频甚低频传播突然扰动~~     

低频甚低频传播突然扰动

SPA1万御(娜)鲡,(牌) SPA VLF仰(邵)SFA1万△A(dB)洲IMP豁(UT)2以X)年 12月 日开始(UT)极大侧叭X(Ul,),本月无观测低频甚低频传播突然扰动~~     

低频甚低频传播突然扰动

2005年开始极大结束级别SPA SPA SFA10月START MAX END I MP LF VLF LF日(UT)(UT)(UT)Δφ(μs)Δφ0(μs)Δφ0(μs)ΔA(dB)本月无电离层扰动事件低频甚低频传播突然扰动     

低频甚低频传播突然扰动

2006年开始极大结束级别SPA SPA SFA2月START MAX END I MP LF VLF LF日(UT)(UT)(UT)Δφ(μs)Δφ0(μs)Δφ0(μs)ΔA(dB)*本月无电离层扰动事件低频甚低频传播突然扰动~~     

低频甚低频传播突然扰动

2006年开始极大结束级别SPA SPA SFA5月START MAX END IMP LF VLF LF日(UT)(UT)(UT)Δφ(μs)Δφ0(μs)Δφ0(μs)ΔA(d*本月无电离层扰动事件低频甚低频传播突然扰动~~     

低频甚低频传播突然扰动

2006年开始极大结束级别SPA SPA SFA10月START MAX END IMP LF VLF LF日(UT)(UT)(UT)Δφ(μs)Δφ0(μs)Δφ0(μs)ΔA(dB)*本月无电离层扰动事件低频甚低频传播突然扰动~~     

低频甚低频传播突然扰动

2006年开始极大结束级别SPA SPA SFA1月START MAX END I MP LF VLF LF日(UT)(UT)(UT)Δφ(μs)Δφ0(μs)Δφ0(μs)ΔA(dB)*本月无电离层扰动事件低频甚低频传播突然扰动~~     

低频甚低频传播突然扰动

2007年开始极大结束级别SPA SPA SFA2月START MAX END IMP LF VLF LF日(U T)(UT)(UT)?φ(μs)?φ0(μs)?φ0(μs)?A(d B)16005801050125U1-1.2-1.9--1.1低频甚低频传播突然扰动~~     

低频甚低频传播突然扰动

2006年开始极大结束级别SPA SPA SFA3月START MAX END I MP LF VLF LF日(UT)(UT)(UT)Δφ(μs)Δφ0(μs)Δφ0(μs)ΔA(dB)*本月无电离层扰动事件低频甚低频传播突然扰动~~     

Flare-time sudden enhancements of low frequency field strength and associated meter wave solar radio bursts

A number of meter wavelength solar radio bursts of spectral Type-III have been observed by means of a solar radio spectroscope (40–240 MHz) simultaneously with sudden enhancements of low frequency (164 KHz) field strength (SES's) of Radio Tashkent which are known to take place due to the enhancements of D-layer ionization caused by flare-time solar X-rays.The association between the solar X-ray flares as detected by the SES's and the Type-III meter-wave solar bursts is discussed. It is found that the association of SES's and meter wave solar bursts, which implies the ejection of flare-time electrons towards the photosphere as well as corona, is about 72%.     

2.6--3.8 GHz太阳微波爆发中的精细结构

根据1994年lslike＆Benz给出的1－3GHz频带上的微波III型爆发和微波尖峰辐射的分类定义,分析北京天文台26－3．8GHz频带上观测到的微波爆发的精细结构．通过分析发现该定义有局限性．本文重新定义了该波段上的微波III型爆发和微波尖峰辐射,并讨论了这种分类定义与设备时间分辨率的关系     

On the generation of high-energy particles in solar flares

This paper discusses the relationship between some characteristics of microwave type IV radio bursts and solar cosmic ray protons of MeV energy. It is shown that the peak flux intensity of those bursts is almost linearly correlated with the MeV proton peak flux observed by satellites near the Earth and that protons and electrons would be accelerated simultaneously by a similar mechanism during the explosive phase of solar flares.Brief discussion is given on the propagation of solar cosmic rays in the solar envelope after ejection from the flare regions.     

MSRT的太阳观测能力

密云米波综合孔径射电望远镜（ ＭＳＲＴ） 是一架同时具有高空间分辨率和高时间分辨率,高灵敏度的大型设备,工作频率在２３２ ＭＨｚ。使用该望远镜能得到太阳爆发的空间分布及其随时间变化的丰富信息,所得数据将填补我国具有空间分辨率的太阳射电数据的空白。在国际太阳活动监测中,由于地理位置原因,也是其它同类设备不可取代的。可以期待在第２３ 周太阳峰年的观测与研究中,得到新的有意义的数据和研究成果     

Synchronous microwave brightenings of solar active regions from RATAN-600 spectral observations

The observations of the solar radio emission on September 11, 2001, with the RATAN-600 radio telescope (southern sector) at four centimeter wavelengths (1.92, 2.24, 2.74, and 3.21 cm) revealed synchronous brightenings in solar radio sources. These were identified on the solar photosphere with active regions that were spaced up to ～10⁶ km apart (AR 9608 and AR 9616). We discuss manifestations of the possible mechanisms of synchronous brightenings in solar sources in a narrow microwave spectral band. The significant linear correlation (ρ_c = 0.84–0.92) between the relative fluxes of AR 9610 and AR 9608 at 1.92 and 2.24 cm and the significant linear correlation (ρ_c = 0.65–0.84) between the relative fluxes of AR 9606 and AR 9608 at 3.21 cm in a two-hour interval of observations are indicative of the interconnection between these active regions not only during flares and bursts, but also in the periods of their absence. This confirms the existence of a large-scale temporal component in the dynamics of the radio flux variations for these active regions. We found a difference between the temporal variations of the radio emission from the halo and the solar radio sources under consideration. The times of increase in the total solar soft X-ray (0.5–4.0 Å, 1.0–8.0 Å; GOES 8, GOES 10) flux are shown to coincide with the times of increase in the fluxes from the solar radio sources at short centimeter wavelengths.     

太阳射电微波爆发及其精细结构研究进展

太阳射电微波爆发携带着爆发源区的物理环境及辐射机制等诸多重要信息。其辐射频段较高，通常来自低日冕磁重联区，尤其是微波爆发的精细结构，持续时间短、变化快、结构复杂，可以反映重联过程复杂的磁场结构、高能粒子运动等许多特征。综述了太阳微波射电爆发分类研究的3个主要阶段，介绍了每一阶段的重要爆发类型、物理机制研究及相应的观测设备，讨论了进一步研究的方向。     

Initial Results of the Ichon Solar Radio Spectrograph

A new solar radio spectrograph to observe solar radio bursts has been installed at the Ichon branch of the Radio Research Laboratory, Ministry of Information and Communication, Korea. The spectrograph consists of three different antennas to sweep a wide band of frequencies in the range of 30 MHz ∼ 2500 MHz. Its daily operation is fully automated and typical examples of solar radio bursts have been successfully observed. In this paper we describe briefly its hardware and data processing methods. Then we present coronal shock speeds estimated for 34 type II bursts from May 1998 to November 2000 and compare them with those from other observatories. We also present the close relationship between onset time of type II bursts and X-ray flares as well as their associations with coronal mass ejections.     

Variations of type III burst parameters during a decametric solar storm

An analysis has been made of type III bursts recorded during a decametric solar storm observed from July 29 to August 16, 1975 with the UTR-2 antenna (Kharkov, IRE Acad. Sci. Ukr. SSR). The bursts were recorded with a dynamic spectrograph and radiometers at 25.0, 20.0, 16.7, and 12.5 MHz. Daily observations have yielded histograms of the type III burst distribution with respect to the frequency drift rate in three subbands between 25.0 and 12.5 MHz. During the middle stage of the storm the drift rate was about twice as high as at the onset and the final stage of the storm. Abrupt changes in the mean frequency drift rate were registered some two to three days after the active region McMath 13790 had come onto the limb and also before it disappeared behind the solar disk. Sudden changes in the drift rates of the type III bursts were accompanied by sudden changes of their mean duration. The rather long burst durations observed at 25.0 MHz at the beginning and the end of the radio storm coincided with such at the twice lower frequency, i.e. 12.5 MHz, during the period when an increased drift rate was observed.Similar variations of type III burst parameters can be interpreted in the framework of the plasma mechanism of burst generation in the corona, assuming that at the middle stage of the storm the bursts observed in the 25.0–12.5 MHz range were emitted at the fundamental whereas when the emitting region was near the limb the bursts received corresponded to the second harmonic of the Langmuir oscillations in the range of 12.5 to 6.25 MHz excited at greater heights.     

太阳射电辐射的自调制模型

本文采用几何光学近似，研究在日冕条件下，沿着磁场传播的电磁波产生非线性自调制不稳定性的可能．发现只有分米波和米波段的射电爆发，可以在日冕外层产生纵向和横向的自调制不稳定性．而在其它波段，如光学、X射线和高频电磁波，则不会产生这样的非线性不稳定性过程．由纵向自调制不稳定性产生的精细结构具有包络孤波的形状．     

Fine structure of large flare radioemission

Several recent phenomena with zebra patterns (ZPs) and fiber bursts on the dynamic spectra of solar type IV radio bursts have been complexly analyzed using all available ground-based and satellite data (SOHO, TRACE, RHESSI). ZPs and fiber bursts were observed at frequencies of 50–3800 MHz. The main relative spectral parameters and the degree of circular polarization of ZPs and fiber bursts are almost identical. The fine structure was observed in powerful and weak phenomena (and was more impressive in weak phenomena) during impulsive and decline phases at instants of recurring continuum bursts. The shape of the fine structure depends on that of the magnetic loops in a radio source, the type of fast particle acceleration (impulsive or prolonged), and the presence of shock waves and coronal mass ejections. Several new effects of the interaction between zebra stripes and fiber bursts have been detected. Specifically, up to 40 fiber bursts with different frequency ranges were simultaneously observed in the frequency range 1–2 GHz against a background of sudden absorptions. It has been indicated that different effects in the ZP stripe behavior can be explained within the scope of the model with whistlers, if the quasi-linear diffusion of fast particles on whistlers (which deforms the particle velocity distribution function) is taken into account.