共查询到20条相似文献，搜索用时 109 毫秒
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钟信号分配放大器的主要用途是把原子钟的10MHz、5MHz、1MHz和1pps信号以高质量的缓冲分别以多路形式不失真地馈送给用户,其目的是:第一,隔离负载对原子钟的影响:第二,在同一原子钟情况下,能向负载提供5路与钟一样的信号。它是高精密时 相似文献
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在多路时频信号的自动测量中,开关系系统是一个不可缺少的组成部分.尽管控制方式有各种各样,但有一个最基本的技术要求——开关系统的隔离度,无论对于一个测量系统的总体设计者或者对于一个开关系统的实际制作者,都必须根据所要求达到或期待的测量目标予以考虑和确定。本文从信号相位和频率测量的角度,探讨了一个开关系统可能对这些测量带来的影响,并力图在测量目标与开关系统隔离度之间导出一定的数学关系。 相似文献
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基于CPLD的高精度可调脉冲信号发生器研制 总被引：1，自引：0，他引：1
为满足精密时间间隔测量设备的测试需要,研制了一种时间间隔可调的高精度脉冲信号发生器。利用计算机串口控制的方式,结合复杂可编程逻辑器件（CPLD）集成度高、可靠性好及工作速度快的优点,采用A1tera公司的设计软件QuartusII进行设计仿真及实现。仿真与实测实验表明,该脉冲信号发生器不仅可以产生单路可调脉冲信号,而且能产生多路可调脉冲信号,产生的单路秒脉冲信号的1s取样Allan方差为1．84×10^-11;产生的时间间隔为100ns的多路脉冲信号的1s取样Allan方差为2．36×10^-11,2路信号之间的时间间隔数据系列的峰一峰值为101ps,可以满足多通道时间间隔测量设备测试要求的稳定度与准确度。 相似文献
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一种双向测距与时间同步系统的设计与分析 总被引：1，自引：0，他引：1
在研究双向单程伪距测量原理的基础上,设计了双向测距与时间同步（DRTS）终端系统总体构架,阐述了在系统中使用的技术,并搭建了基于DSP＋FPGA的双向测距与时间同步系统软硬件平台。实验结果表明,此系统的码速率为5MHz、中心频率为15MI-Iz时,测距和时间同步的分辨率可达0．15cm和5ps（@1S）,采用不同频率源时测距和时间同步的精度分别为1．038m和3．46ns,采用相同频率源时分别为0．28cm和9．43ps（参考频率稳定度1×10^-10／d量级）。与国外同类产品相比具有测量精度优势,但考虑通用性,此系统的硬件仍需进一步优化,软件上需要做到码速率可调。 相似文献
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晚型星计算机自动光谱分类 总被引：1，自引：1，他引：0
在对恒星形成区（ＳＦＲ）中ＲＯＳＡＴ选弱发射线Ｔ Ｔａｕｒｉ星（ＷＴＴＳ）进行光谱证认的过程中,发展了一套基于北京天台２．１６米光学望远镜及其ＯＭＲ卡焦光谱仪系统的晚型星中色散（５０Ａ／ｍｍ）光谱计算机自动光谱分类方法。对ＲＯＳＡＴ选ＷＴＴＳ候选体中晚型星进行自动光谱分类的结果表明,一般情况下,光谱型的分类精度可达±１个次级,个别源为±２个次级。该自动光谱分类方法同时适用于其它光谱晚型星。 相似文献
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北京天文台自1986年开始高时间分辨率的六厘米波段强度干涉仪的研制,计划在北京、昆明、乌鲁木齐设三个站,可发现角经0.01″的源。1988年初完成了北台单站接收系统,并取得了部分观测资料。主要性能如下:天线口径1.5米;接收频率5070±50MHz;高放噪声温度150K;中放带宽40MHz;系统时间常数0.2μs。系统见图1。采用前置微波高放未提高系统的灵敏度。用气体放电噪声管加15db定向耦合器组合作噪声标准源,以噪声源的输出温度为单位来测量每天的太阳强度m,由多日积累的m_i(i=1……n)与SGMR 4995MHz(引自S.G.D)的值取相关得线性相关参数a、b。由此得每天的绝对流量。目前只是初步的结果。表1为逐日的太阳射电强度m;SGMR 4995MHz;y;及黑子相对数Y。图2为V—m及y—m相关图,图上为S_p、S_n、Y及y的逐日变化图。表2为巡视观测中记录的部分爆发。六厘米强度干涉仪已取得的结果显示与太阳射电的国际频谱有很好的相关。三站(北京、昆明、乌鲁木齐)的强度干涉仪网建立后(1990年)所取得的高时间分辨率爆发的精细结构将具有极好的可靠性。该网将参加全国性的太阳活动联测。 相似文献
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介绍了BPM短波授时信号模拟器的主要功能和工作原理,阐述了该模拟器的系统组成、输入输出及软件流程。该模拟器以GPS信号作为时间源,以10 MHz的高稳定恒温晶振作为守时频率源,并在程序控制下产生载频与调制信号,放大输出6路BPM短波模拟信号。测试结果表明,该模拟器的功能与技术指标符合BPM短波授时信号的要求。 相似文献
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Jin Sheng-zhen Li Xiao-cong Ji Hui-rong Zhao Bing Wang Shu-lan Yan Yuan-yi Zhao Ren-yang 《Chinese Astronomy and Astrophysics》1993,17(4):406-412
We briefly describe the polarization state of the spike groups and fast fine structures superimposed on the 47GB microwave burst of 1991 May 16. At two frequencies 100 MHz apart, namely, 2645 and 2545 MHz, the polarization showed rapid reversals on short time scales of the order of 50 100ms. We think this is probably related to fluctuations on both short time and small spatial scales, in the plasma density and magnetic field of the emission region. Thése oscillations cause the plasma and cyclotron frequency ratio to vary around the value of
, thus making the electron cyclotron maser instability growth rate to be dominated alternately by the X mode and the O mode and the polarization state to switch from one sign to the other. 相似文献
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Two remarkable intensity-time patterns in the 113 and 64 MHz single-frequency radio flux records during a type I noise storm and/or a type IV burst on 31 July, 1983 are studied. A comparison of the patterns at both frequencies reveals a high degree of resemblance and inherent common structure although the 64 MHz pattern was seen 40 min later than the 113 MHz pattern. An interpretation is given assuming a slowly uprising and thereby expanding clumpy plasma-magnetic field configuration which is (via accompanying coronal loops) two times illuminated by energetic electrons coming from the soft X-ray flare precursor source region of the H-alpha flares F1 and F2 (see Figure 1). 相似文献
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J. D. Mathews S. J. Briczinski D. D. Meisel C. J. Heinselman 《Earth, Moon, and Planets》2008,102(1-4):365-372
Radio science and meteor physics issues regarding meteor “head-echo” observations with high power, large aperture (HPLA) radars,
include the frequency and latitude dependency of the observed meteor altitude, speed, and deceleration distributions. We address
these issues via the first ever use and analysis of meteor observations from the Poker Flat AMISR (PFISR: 449.3 MHz), Sondrestrom
(SRF: 1,290 MHz), and Arecibo (AO: 430 MHz) radars. The PFISR and SRF radars are located near the Arctic Circle while AO is
in the tropics. The meteors observed at each radar were detected and analyzed using the same automated FFT periodic micrometeor
searching algorithm. Meteor parameters (event altitude, velocity, and deceleration distributions) from all three facilities
are compared revealing a clearly defined altitude “ceiling effect” in the 1,290 MHz results relative to the 430/449.3 MHz
results. This effect is even more striking in that the Arecibo and PFISR distributions are similar even though the two radars
are over 2,000 times different in sensitivity and at very different latitudes, thus providing the first statistical evidence
that HPLA meteor radar observations are dominated by the incident wavelength, regardless of the other radar parameters. We
also offer insights into the meteoroid fragmentation and “terminal” process. 相似文献
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光纤时间传输及相位补偿 总被引：2，自引：0，他引：2
介绍了国外几种利用光纤进行时间频率传递的方法和经验.对无补偿光纤时间频率传递方法、双向时间频率传递方法、光学机械温度补偿方法及电子共轭相位补偿方法作了较详细的描述.光纤时延主要随温度而变化,在200 km以内,时延的日变化为几纳秒,月变化为十几纳秒.在50 km内利用光纤传输100 MHz频率信号时,在不补偿情况下频率稳定度为: 3×10-14/s,1×10-15/d;光学补偿后的频率稳定度可达到1.5×10-14/s,1×10-17/d.电子共轭相位补偿后,温度变化20℃引起的相位变化降低了45倍.光纤传输对短期频率稳定度影响较小,对日及更长期的频率稳定度影响较大. 相似文献
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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
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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
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K. S. Dwarakanath R. K. Shevgaonkar Ch. V. Sastry 《Journal of Astrophysics and Astronomy》1982,3(2):207-216
We have observed the extended supernova remnants HB 9 (G 160.5 + 2.8) and IC 443 (G 189.1 + 2.9) at 34.5 MHz with a resolution
of 26 arcmin × 40 arcmin. A map of HB 9 is presented. The integrated flux density of HB 9 at 34.5 MHz is 750 ± 150 Jy. The
spectral index in the frequency range from 34.5 MHz to 2700 MHz is found to be constant (- 0.58 ± 0.06) without any spectral
break such as was reported earlier by Willis (1973). There is no significant variation of the spectral index across the remnant.
The integrated flux density of IC 443 at 34.5 MHz is 440 ± 88 Jy. The spectral index in the frequency range from 20 MHz to
10700 MHz is - 0.36 ± 0.04. The reduction in flux at very low frequencies (10 MHz) is attributable to free-free absorption
in the interstellar medium and/or in the H II region S 249. 相似文献
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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
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S. Ya. Braude A. V. Megn B. P. Ryabov I. N. Zhouck 《Astrophysics and Space Science》1970,8(2):275-322
On the basis of the absolute measurements in the 12.6–25 MHz frequency range and the relative measurements at frequencies 750, 1400, 2695 and 5000 MHz (NRAO) and 408, 1410 and 2650 MHz (Parkes), 57 standard spectra were obtained which are linear (on a log-log scale) in the range 12.6–5000 MHz. The comparison of the flux densities presented in the surveys at 10.03, 22.25, 26.3, 38, 86 and 178 MHz and the standard spectra was carried out and thus the correction coefficient was calculated. It was shown that the scale of absolute fluxes CKL on the frequencies 38 and 178 MHz is lowered on 28% and 8% respectively. The possible sources of divergences of the results of measurements in decametric wavelength is discussed. Making use of the corrected data at 38 MHz and 178 MHz, of the results at higher frequencies mentioned above and of the original results of measurements in the 12.6–25 MHz range, the spectra of 55 discrete sources were constructed. The spectra of 149 sources are also obtained on the basis of the surveys at 10.03, 22.25, 26.3, 38 and 178 MHz corrected according to standard spectra. 相似文献