22.6--3.8 GHz 太阳射电动态频谱仪

给出北京天文台 ２．６—３．８ ＧＨ_(ｚ)太阳射电动态频谱仪的性能、结构及初步观测结果．     

1—2GHz太阳射电动态频谱仪

本描述了北京天台研制的１－２ＧＨｚ太阳射电动态频谱仪的性能，结构，初步观测结果及进一步改进计划。     

太阳射电宽带动态频谱仪步研究进展

介绍了围绕我国近年完成的太阳射电宽带动态频亦仪展开的研究工作进展，并提出了今后的努力方向，以期庐设备能在我国第23周太阳活动峰年研究中发展更大作用。     

紫金山天文台4.5-7.5 GHz太阳快速频谱仪图像

运用多种方法，对紫金山天文台4．5—7．5GHz太阳快速频谱仪获得的太阳微波爆发频谱图像进行后续处理，尽可能地去除噪声和干扰，还原爆发事件的本来面目，并突出感兴趣的部分，在MATLAB的平台支持下编写了WINDOWS下的应用软件，取得了较为满意的结果．     

云南天文台太阳射电频谱仪的网络系统

介绍云南天文台太阳射电米波（２３０～３００ＭＨz）、分米波（０．７～０．４ＧＨz）频谱观测系统及１０m射电望远镜自动控制系统“星型拓扑”对等网的建立。该网络,不但 实现了光盘刻录机、激光打印机等资源共享,而且还为解决由于太阳射电频谱高时间分辨率和高频率分辨率观测带来的大数据量处理和存储找到了解决途径。     

微波Ⅲ型爆发在1—2GHz太阳射电快速频谱仪上的观测

叙述了１９９７年１月至１９９８年４月,使用北京天台７ｍ射电望远镜在１－２ＧＨｚ频率上观测的微波Ⅲ型爆发的分析结果。共分析６０个事件,获得了单峰、多峰、群集和负吸收微波Ⅲ型爆发的四种型别。通过对它们的频宽、频漂、偏振等重要参量的分析,初步得出微波Ⅲ型爆发在１－２ＧＨｚ上的一些基本特性。     

太阳射电频谱仪数据采集与自理自相关频谱仪原理与应用）

本文论述了０．７～１．４ＧＨz太阳射电频谱仪数据采集与处理系统是如何实现的。正在 研制的此仪器采用了多通道频谱仪与自相关频谱仪结合使用的方案。首先,本文详细讨论了自相关频谱仪的原理,并介绍了北京大学研制的自相关频谱仪的结构。在此基础上着重讨论了多通道频谱仪与自相关频谱仪的同步控制的解放方案,以及大容量数据采集实时存盘的解决方案。最后,介绍了我们为数据预处理采用的一些方案。     

太阳射电频谱仪超高时间分辨率观测的新结果

国家天文台分米波太阳射电频谱仪用新的观测模式获得太阳射电频谱的一些新的观测现象。新的观测模式频率在1．1—1．34GHz范围，时间分辨率是1．25ms；正常的观测模式下频率在1．1—2．06GHz范围，时间分辨率是5ms。在两种模式下频率分辨率为4MHz。发现窄带Ⅲ型爆发（“blips”）斑马纹（Zebra）和纤维结构（Fiber）中的超精细结构和一些新的精细结构。这些新的结果有助于深入理解在太阳耀斑期间低日冕中能量的释放和转移，也为拟建中的太阳射电频谱日像仪提出了新的要求。     

云台射电频谱仪预研

简要介绍了用于研究分子夭文学的各种射电频谱仪及国内外发展状况,讨论了各种频谱仪的优缺点,最后提出了云台建立射电频谱仪的型式。     

Some Observed Results of Solar Radio Spectrometer at 4.5—7.5GHz

A new instrument of broadband solar radio spectrometer working at waveband 4.5-7.5GHz was developed at Purple Mountain Observatory for Solar Maximum 23. Some new results of spectral observation have been obtained since August 1999.Two typical type Ⅲμbursts with rich fine structures are presented and some interesting features discussed.     

A New Solar Radio Spectrometer at 1.10-2.06 GHz and First Observational Results

An improved Solar Radio Spectrometer working at 1.10-2.06 GHz with much improved spectral and temporal resolution, has been accomplished by the National Astronomical Observatories and Hebei Semiconductor Research Institute, based on an old spectrometer at 1-2 GHz. The new spectrometer has a spectral resolution of 4 MHz and a temporal resolution of 5ms, with an instantaneous detectable range from 0.02 to 10 times of the quiet Sun flux. It can measure both left and right circular polarization with an accuracy of 10% in degree of polarization. Some results of preliminary observations that could not be recorded by the old spectrometer at 1-2 GHz are presented.     

A Solar Radio Spectrometer at 5.2–7.6 GHz

The properties, structure and performance of a Solar Radio Spectrometer working at 5.2–7.6 GHz developed by National Astronomical Observatories/Beijing and Hebei Semiconductor Research Institute are described. The spectrometer has a spectral resolution of 20 MHz and a temporal resolution of 5 ms, with an instantaneous detectable range from 2% to 10 times flux of the quiet Sun. It can measure both left and right circular polarizations with an accuracy of 10% of polarization degree. Some results of preliminary observations are presented.     

A Broadband Solar Radio Spectrometer and Some New Observational Results

A broadband solar radio spectrometer with a bandwidth of about 7 GHz has been developed in China for solar maximum 23. This work is a cooperative project of Beijing Astronomical Observatory (BAO), Purple Mountain Observatory (PMO), Yunnan Observatory (YNO), and Nanjing University. The spectrometer of PMO worked in the waveband of 4.5–7.5 GHz, that of BAO in 1–2 GHz, 2.6–3.8 GHz, and 5.2–7.6 GHz, and that of YNO in 0.7–1.5 GHz. The spectrometer of PMO is a multichannel and frequency-agile one with a time resolution of 1–5 ms and a frequency resolution of 10 MHz. It started to operate in August 1999 and since then more than 300 spectral events have been observed, and some type III or type III-like structures have also been found. In this paper, some selected typical events, for example, the events on 25 August 1999 and 27 October 1999, are presented, and some new observed features are also described and discussed.     

1．35cm太阳射电缓变事件与可能的辐射机制

１９９３年５月３０日２２ＧＨｚ的缓变型射电事件的时间轮廓特征，以及在３ＧＨｚ、１０ＧＨｚ频率上没有对应射电事件的观测特征等，可用Ｍａｔｚｌｅｒ的热模型得到合理的解释。     

A New Solar Broadband Radio Spectrometer (SBRS) in China

A new radio spectrometer, Solar Broadband Radio Spectrometer (SBRS) with characteristics of high time resolution, high-frequency resolution, high sensitivity, and wide frequency coverage in the microwave region is described. Its function is to monitor solar radio bursts in the frequency range of 0.7–7.6 GHz with time resolution of 1–10 ms. SBRS consists of five `component spectrometers' which work in five different wave bands (0.7–1.5 GHz, 1.0–2.0 GHz, 2.6–3.8 GHz, 4.5–7.5 GHz, and 5.2–7.6 GHz, respectively). A combination of multi-channel and scanning techniques is adopted. The component spectrometers are attached to different antennas which are separately located at Beijing, Kunming, and Nanjing. Close attention was paid to solve the problems of sensitivity, dynamic range, interference-resistance, data acquisition, and handling a large amount of data. The SBRS was put into operation in the 23th solar maximum activity period, and has proved itself to be a valuable instrument for the study of solar bursts in microwaves.     

太阳射电频谱仪数据采集与处理(自相关频谱仪原理与应用)

本文论述了 0 .7～ 1 .4GHz太阳射电频谱仪数据采集与处理系统是如何实现的。正在研制的此仪器采用了多通道频谱仪与自相关频谱仪结合使用的方案。首先 ,本文详细讨论了自相关频谱仪的原理 ,并介绍了北京大学研制的自相关频谱仪的结构。在此基础上着重讨论了多通道频谱仪与自相关频谱仪的同步控制的解决方案 ,以及大容量数据采集实时存盘的解决方案。最后 ,介绍了我们为数据预处理采用的一些方案。     

2840MHz太阳射电辐射流量计的升级改造

叙述了国家天文台升级改造后的2 840 MHz太阳射电辐射流量计的设计特点、性能、结构及观测结果。升级改造后的太阳射电辐射流量计将在较高时间分辨率上实时得到2 840 MHz频率上的太阳流量,为太阳物理研究积累丰富的观测数据,是太阳活动监测和预报的重要参数之一。     

Eruptive Solar Prominence at 37 GHz

On 27 June 2012, an eruptive solar prominence was observed in the extreme ultraviolet (EUV) and radio wavebands. At the Aalto University Metsähovi Radio Observatory (MRO) it was observed at 37 GHz. It was the first time that the MRO followed a radio prominence with dense sampling in the millimetre wavelengths. This prompted us to study the connection of the 37 GHz event with other wavelength domains. At 37 GHz, the prominence was tracked to a height of around \(1.6~\mathrm{R}_{\odot}\), at which the loop structure collapsed. The average velocity of the radio prominence was \(55 \pm 6~\mbox{km}\,\mbox{s}^{-1}\). The brightness temperature of the prominence varied between \(800 \pm 100\) K and \(3200 \pm 100\) K. We compared our data with the Solar Dynamic Observatory (SDO)/Atmospheric Imaging Assembly (AIA) instrument’s 304 Å EUV data, and found that the prominence behaves very similarly in both wavelengths. The EUV data also reveal flaring activity nearby the prominence. We present a scenario in which this flare works as a trigger that causes the prominence to move from a stable stage to an acceleration stage.