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1.
在磁拱底部非线性等离子体密度波传播期间,损失锥分布的反射电子驱动着电子迴旋maser不稳定性的增长,激励出二次谐频波模,支配着太阳射电毫秒Spike辐射。根据这个理论模型,本文着重研究了太阳射电毫秒Spike辐射的频带宽度问题。对于典型参数,计算结果发现:辐射带宽一般为几MHz到几十MHz,最高为100MHz。而且通常折射出的二次谐频z模辐射带宽较窄,而二次谐频o模辐射带宽较宽。 相似文献
2.
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
3.
本文简要地叙述了1990年7月30日伴随日面2B级光学耀斑发生的射电爆发,在2840、2640、和1420MHz波段上同步观测结果,其中包括射电爆发在以上波段的秒级时间轮廓和毫秒级时间尺度的spike辐射活动.对它们的形态和频率特征作了简要分析,同时对spike辐射的迴旋电子脉塞增长率、相对辐射频宽和准周期振汤的某些特征及辐射源区的某些物理参数,作了进一步的分析和量级的估算. 相似文献
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5.
本文给出了不同能谱指数Γ的非热电子,在不同传播方向的迴旋同步加速辐射的发射因子h_(1,2)(s,θ)的详细结果。其结果表明,对同一谐波数s而言,h_(1,2)(s,θ)随着θ值(波矢量k与磁场方向Η的夹角)的增加或Γ值的下降而增加,而对同一θ和Γ值而言,h_(1,2)(s,θ)还随着s 的增加而迅速下降,而当Γ=1时,h_(1,2)(s,π/2)随着s的增加而下降的程度十分缓慢,表明在横传播条件下,非热电子具有比似纵传播高得多的发射能力,其相应的辐射流量密度要比似纵传播高出几倍。 采用 Sturrock 的耀斑爆发源模型,计算了θ=π/2情况下的迴旋同步加速辐射的射电爆发谱。我们发现对具有Γ=1的非热电子的低次谐波辐射,分别在Ⅳ型爆发的300MHz和9000MHz附近有个峰值,而在他们的高频端的低次谐波的迴旋同步加速辐射遭到强烈的迴旋共振吸收而使辐射迅速下降,从而形成两峰一谷的U型射电爆发谱。 计算表明,1972年8月4日的大爆发,很可能是一团具有能谱指数为1.5,总数为10~(32)—10~(34)的非热电子,在横传播条件下的迴旋同步加速辐射和热电子的迴旋共振吸收机制产生的。 相似文献
6.
黄光力 《中国天文和天体物理学报》1993,(1)
本文在用MHD理论研究等离子体束流不稳定性时发现:在电子等离子体频率附近可以激发出宽频带电磁波,其时间尺度、方向性、相对带宽、偏振特性及谐波结构等理论预期,在典型的日冕参数下,和米波段太阳射电Ⅲ型爆发的观测结果基本吻合.这一机制还可避免经典的等离子体辐射理论中由Langmuir波转换成横电磁波的效率较低的主要困难. 相似文献
7.
在中子星磁轴吸积柱的上部,少数高能电子通过磁镜点反射,可使部份电子的速度分布形成非热分布,由此激发激射(Maser)不稳定性。波被放大,发射出频率近似为电子迴旋频率及其倍频的相干辐射。用此模型计算了HerX-1的迴旋线发射。发现不稳定性增长率与吸积柱中电子数密度成正比,因而比非相干散射产生的连续辐射随电子数密度增长更快;而且发射线的强度和能量均与脉冲相位关联。这个理论可解释近期的HerX-1观测结果。 相似文献
8.
自1990年6月北京天文台太阳射电偏振仪投入实测以来,观测到一百多个“Spike”和短时标精细结构微波幅射,其中包括一些新的微波幅射特征。本文给出了主要的四点特征:(1)窄带辐射;(2)快速偏振逆转;(3)快速频率漂移;(4)不同时标的准周期振荡。 相似文献
9.
弱磁化相对论电子束注入等离子体时，由非共振波粒相互作用激发的束－等离子体不稳定性可以直接放大电磁波，计算结果表明：在偏离共振条件的区域，电磁波仍可在较宽的频率范围被放大，并在每个共振峰下形成平台结构。随着谐波数的增高，增长率峰值逐渐变小，峰宽也变窄。本文还分析了电磁波的增长率随背景参数ω＿（ｐｅ）／Ω＿ｅ及高能电子的入射方向和辐射方向的变化规律，在典型的日冕条件下，此类不稳定性所放大的电磁波的增长率大小、带宽、方向性、偏振及谐波等性质，可以用来解释太阳Ⅲ型射电爆发现象，本文的研究亦可用来解释其他天体等离子体辐射。 相似文献
10.
太阳射电尖峰辐射(spike)的窄频带是一个具有特征性的参数,不但可从它计算出Spike辐射源区的小尺度结构,而且观测结果与Spike辐射理论可相互验证.我们利用云南天文台0.5 MHz频率分辨率的射电频谱观测资料,作出了230—300MHz频段上单个Spike带宽分布,并由此给出一群Spike源区的最可几尺度为151km,最大源区尺度为830km. 相似文献
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L.M. Erukhimov A.M. Lerner V.I. Kosolapenko E.N. Myasnikov 《Planetary and Space Science》1981,29(9):931-933
The spectra of amplitude fluctuations have been determined using 400 MHz transmissions from the Navy navigation satellite system (NNSS) observed at Spitsbergen. A spectrum model for electron density fluctuations is discussed. It is shown that a typical spectrum cut-off scale is l011 ～5 + 15 km in the direction of the geomagnetic field. 相似文献
13.
Between 1980, January 1 and 1981, December 31 a total of 664 decimetric pulsation events, abbreviated DCIM, were observed with the Zürich spectrometers in the frequency range 100 to 1000 MHz. All of these events were recorded on film, allowing an effective resolution in time of 0.5 s, and 5 MHz in frequency. Some of these events were also recorded digitally with higher time and frequency resolution.The class of DCIM bursts can be divided into two groups depending on their duration and thus reflecting different physical mechanisms. Each of the two groups can be further divided into small and large bandwidth subgroups, reflecting differences in the source parameters. Short decimetric events ( 1s) are most abundant in this frequency range. They may be caused by fast transients in the solar atmosphere. The half-power bandwidth of the shortest DCIM bursts, the millisecond spikes, were found to be 6 to 12 MHz. A single event may consist of more than 1000 individual spikes. The long lasting DCIM bursts (5 s to 300 s) exhibit a gradual and smooth time profile. Such long lasting events indicate the presence of trapped particles in magnetic fields. In some events decimetric gyrosynchrotron radiation was observed below 1000 MHz as a continuation of corresponding microwave events.Some of the decimetric events exhibit very large drift rates (2000 MHz s-1). Such large values request either a drastic reduction of the effective scale height of the active region in the beam model or a different explanation than the conventional beam model. 相似文献
14.
We present the results of the analysis of thirteen events consisting of dm-spikes observed in Toruń between 15 March 2000
and 30 October 2001. The events were obtained with a very high time resolution (80 microseconds) radio spectrograph in the
1352 – 1490 MHz range. These data were complemented with observations from the radio spectrograph at Ondřejov in the 0.8 – 2.0 GHz
band. We evaluated the basic characteristics of the individual spikes (duration, spectral width, and frequency drifts), as
well as their groups and chains, the location of their emission sources, and the temporal correlations of the emissions with
various phases of the associated solar flares. We found that the mean duration and spectral width of the radio spikes are
equal to 0.036 s and 9.96 MHz, respectively. Distributions of the duration and spectral widths of the spikes have positive
skewness for all investigated events. Each spike shows positive or negative frequency drift. The mean negative and positive
drifts of the investigated spikes are equal to −776 MHz s−1 and 1608 MHz s−1, respectively. The emission sources of the dm-spikes are located mainly at disk center. We have noticed two kinds of chains,
with and without frequency drifts. The mean durations of the chains vary between 0.067 s and 0.509 s, while their spectral
widths vary between 7.2 MHz and 17.25 MHz. The mean duration of an individual spike observed in a chain was equal to 0.03 s.
While we found some agreement between the global characteristics of the groups of spikes recorded with the two instruments
located in Toruń and Ondřejov, we did not find any one-to-one relation between individual spikes. 相似文献
15.
A group of centimetric spikes was detected during the burst of 10 March 2002 with the spectrometer of NAOC (National Astronomical Observatories of China). These centimetric spikes are resolved clearly in the time and frequency panels. A statistical analysis shows that these spikes have very short durations (5–10 ms), narrow bandwidths (20–40 MHz), very high polarization degrees (≥90%), and relatively weak flux densities (10–40 sfu). The simultaneous 2D image observations of NoRH (Nobeyama Radioheliograph) and SSRT (Siberian Solar Radio Telescope) imply that the spikes should come from a small source region, which was located in an area with a complex magnetic field. It is also found that the spikes are polarized in the X-mode. These observations suggest that the electron cyclotron maser (ECM) is the most likely mechanism of these centimetric spikes. 相似文献
16.
A group of centimetric spikes was detected during the burst of 10 March 2002 with the spectrometer of NAOC (National Astronomical Observatories of China). These centimetric spikes are resolved clearly in the time and frequency panels. A statistical analysis shows that these spikes have very short durations (5–10 ms), narrow bandwidths (20–40 MHz), very high polarization degrees (≥90%), and relatively weak flux densities (10–40 sfu). The simultaneous 2D image observations of NoRH (Nobeyama Radioheliograph) and SSRT (Siberian Solar Radio Telescope) imply that the spikes should come from a small source region, which was located in an area with a complex magnetic field. It is also found that the spikes are polarized in the X-mode. These observations suggest that the electron cyclotron maser (ECM) is the most likely mechanism of these centimetric spikes. 相似文献
17.
Radio spikes and the fragmentation of flare energy release 总被引：1，自引：0，他引：1
A. O. Benz 《Solar physics》1985,96(2):357-370
Decimetric radio events with large numbers of spikes during the impulsive phase of flares have been selected. In the observing range of 100 to 1000 MHz some flares have of the order of 10000 spikes or more. The average half-power bandwidth of spikes has been measured to be only 1.5% of the spike frequency. Since the emission frequency is determined by some source parameter (such as plasma frequency or gyrofrequency) the source dimension must be a small fraction of the scale length. From the flare configuration a typical upper limit of the dimension of 200 km is found. The observed fragmentation in the radio emission cannot be explained by a patchy emission mechanism of a single and much larger source without an additional (and unknown) assumption. It is proposed that the fragmentation already occurs in the exciter.Four events were analyzed in detail and compared to UV, SXR, and HXR data. The density of the loops where the SXR and HXR emission was observed has been measured before the flare. The plasma frequency well agrees with the observed frequency of spikes. The spikes thus originate close to or in the energy release region. It is suggested here that the fragmentation of the exciter is due to a fragmentation of the primary energy release. Each of these 104 microflares would release an energy of the order of 1026 erg within 0.05 s. 相似文献
18.
The characteristics of the millisecond spikes with short duration and weak flux density which were observed with high time resolution (1 ms) at 1420, 2000 and 2840 MHz during the great type IV solar radio burst of 30 July 1990 are introduced in detail in this article. The time profiles of the spikes are statistically analyzed and the parameters of the spike source are also estimated. 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.
Arnold O. Benz Christian Monstein Michael Beverland Hansueli Meyer Bruno Stuber 《Solar physics》2009,260(2):375-388
A new multichannel spectrometer, Phoenix-3, is in operation having capabilities to observe solar flare radio emissions in the 0.1?–?5 GHz range at an unprecedented spectral resolution of 61.0 kHz with high sensitivity. The present setup for routine observations allows measuring circular polarization, but requires a data compression to 4096 frequency channels in the 1?–?5 GHz range and to a temporal resolution of 200 ms. First results are presented by means of a well observed event that included narrowband spikes at 350?–?850 MHz. Spike bandwidths are found to have a power?–?law distribution, dropping off below a value of 2 MHz for full width at half maximum (FWHM). The narrowest spikes have a FWHM bandwidth less than 0.3 MHz or 0.04% of the central frequency. The smallest half-power increase occurs within 0.104 MHz at 443.5 MHz, which is close to the predicted natural width of maser emission. The spectrum of spikes is found to be asymmetric, having an enhanced low-frequency tail. The distribution of the total spike flux is approximately an exponential. 相似文献