共查询到18条相似文献,搜索用时 171 毫秒
1.
星载原子钟是决定星上时间基准的基础。利用一年的事后精密钟差数据,对北斗三号(BDS-3)和其他全球卫星导航系统的准确度、漂移率和稳定度进行了分析,以评估全球卫星导航系统(GNSS)在轨原子钟性能。结果表明:BDS-3的铷原子钟准确度在2.62×10-13~2.54×10-11之间,氢原子钟在1.64×10-14~6.77×10-11之间;BDS-3氢原子钟的漂移率显著优于铷原子钟;BDS-3多数氢原子钟的稳定度可达到10-15量级。BDS-3的稳定度表现最好,其次是全球定位系统(GPS)、北斗二号(BDS-2)、伽利略(Galileo)和格洛纳斯系统(GLONASS)。 相似文献
2.
3.
卫星钟在轨性能评估对于卫星钟差预报与系统完好性监测具有重要作用。利用国际GNSS服务组织发布的事后GPS精密卫星钟差数据,基于频率准确度、漂移率、万秒稳定度及天稳定度对GPS Block IIR、IIR-M、IIF与IIIA 4类卫星的星载钟性能进行评估。结果表明:1) GPS卫星钟的频率准确度与天漂移率分别在10-13~10-12量级与10-15~10-14量级;2) 星载铷钟的万秒稳定度与天稳定度分别可达10-14与10-15量级,比星载铯钟的同类指标高近一个数量级;3) 新型Block IIIA卫星的星载钟的天稳定度比另外3种类型卫星的星载钟的天稳定度更高,达到(3~5)×10-15的水平;4) 无论对于不同系列卫星还是同一系列卫星,各星载钟之间均存在一定的性能差异,这种差异与卫星钟在轨运行时间长短无显著关系。 相似文献
4.
设计并实现了一种用于铷原子频标的小型化锁频环路。采用数字锁相倍频技术,实现了10MHz信号的45.5645833次倍频。再经过一级15次倍频后获得频率为6834.6875MHz的铷原子频标微波探寻信号。通过数字电路技术实现了455.645833MHz信号的小调频。测量并分析了455.645833MHz信号的相位噪声,结果表明电路系统对铷频标频率稳定度的贡献为3.2×10-12τ-1/2。测量了利用该电路得到的铷频标的短期频率稳定度,结果为5×10-12τ-1/2(1s≤τ≤100s),明显高于一般商品小型化铷原子频标。 相似文献
5.
原子时标TA(NIM)是一个独立时标,其频率由NIM5铯喷泉基准驾驭。产生时标的主钟是一台主动型氢原子钟,铯喷泉基准定期对其测量和校准。时标算法通过预估氢钟将来的频率,补偿过去预估频率与校准频率之差,并评估无校准数据期间的氢钟频率,最终尽可能实现TA(NIM)的频率与NIM5铯喷泉基准保持一致。2007年8月,TA(NIM)开始试运行,2008年6月正式运行。1年多来的数据分析表明,TA(NIM)运行连续可靠,与TAI间的时间稳定度(5天)达到1.2 ns,相对频差为2.0×10-15。 相似文献
6.
报道了一种基于光学锁相环的高稳定度激光稳频方法,用于提高可调谐外腔半导体激光器(TECDL)的频率稳定度和准确度。自行研制的光学锁相环电路采用数字鉴相与差分运算相结合的方式获得高灵敏度的鉴频鉴相误差信号,并通过高速模拟PID实现整个系统的闭环锁定。利用该光学锁相环系统进行了TECDL偏频锁定至光学频率梳(OFC)的实验,实验结果表明环路锁定后拍频频率波动在±0.3Hz范围内,偏置频率为50MHz时,光学锁相环系统在1s和1000s积分时间的相对阿伦方差分别为1.5×10-9和8.5×10-13。系统锁定后,拍频线宽由500kHz压缩至2kHz。该研究表明采用基于光学锁相环的激光稳频方法可以实现亚Hz级的激光频差控制,通过将TECDL偏频锁定至高稳定度的参考激光源可显著提高其频率稳定度,使其能够满足超精密测量、冷原子/离子干涉测量等领域对激光频率稳定度和准确度的要求。 相似文献
7.
8.
9.
10.
11.
Prestage J.D. Tjoelker R.L. Wang R.T. Dick G.J. Maleki L. 《IEEE transactions on instrumentation and measurement》1993,42(2):200-205
The frequency stability of an atomic standard based on 199 Hg+ ions confined in a hybrid RF/DC linear trap is described. The 40.5-GHz clock transition has been measured to be 17 mHz wide, representing a quality factor greater than 2×1012. A 160-mHz line is used to steer the output of a 5-MHz crystal oscillator to obtain a stability of 2×10-15 for 24000-s averaging times. In a separate measurement, a 37-mHz line is used to steer the output of the superconducting cavity maser oscillator to reach 1×10-15 stability at 10000 s 相似文献
12.
Sato K. Hara T. Kuji S. Asari K. Nishio M. Kawano N. 《IEEE transactions on instrumentation and measurement》2000,49(1):19-24
An ultrastable fiber optic frequency distribution system is described. The ultrastable phase stability is achieved by configuring a closed phase-locked loop with a single-mode optical fiber transmission line in which two optical carrier signals with different wavelengths are transmitted as a forward and a backward signal, and installing an optical delay control module which has no differential dispersion effect between the two optical carrier waves and induces no electrical noise. A phase stabilized optical fiber (PSOF) is used for the signal transmission line. The stabilities of this system are 7.5×10-17 and 1.1×10-17 in Allan standard deviation at 1000 and 10000 s averaging time, respectively, while the environmental temperature of the PSOF cable varies as much as the range of 10°C and the rate of 10°C/12 h 相似文献
13.
Jinquan D. Xiwen Z. Yuanhai X. 《IEEE transactions on instrumentation and measurement》1993,42(3):755-758
Experiments on the 87Rb maser with both ends pumping showed variations of the maximum output power versus cell temperature. The largest output power was 2.0×10-10 W, and a preliminary measurement gave an improved short-term frequency stability. The results of the numerical calculations based on the density matrix formalism agreed qualitatively with the experiments 相似文献
14.
Luiten A.N. Mann A.G. Costa M.E. Blair D.G. 《IEEE transactions on instrumentation and measurement》1995,44(2):132-135
Microwave oscillators of exceptional short-term stability have been realized from cryogenic sapphire resonators with loaded Q factors in excess of 109 at 11.9 GHz and 6 K. This has been achieved by a power stabilized loop oscillator with active Pound frequency stabilization. These oscillators have exhibited a fractional frequency stability of 3-4×10-15 for integration times from 0.3 to 100 s. The relative drift of these two oscillators over one day is a few times 10-13. To reduce the long-term drift, which is principally due to excessive room temperature sensitivity, we have added cryogenic sensors for the power and frequency stabilization servos to one of these oscillators. We have also implemented a servo to reduce the room temperature sensitivity of our phase modulators. Testing of this oscillator against a Shanghai Observatory H-maser has shown an Allan deviation of 4×10-15 from 600 to 2000 s 相似文献
15.
The CO2 lasers, frequency stabilized on OsO4 transitions around 29 THz, are successfully used as secondary references for visible frequency synthesis and also for high-accuracy spectroscopy in the infrared domain. The BNM-LPTF CO2/OsO4 frequency standards exhibit high metrological performances: a long term reproducibility of ±10 Hz (1σ=2×10-13) and a stability σy=6.6×10-14/√τ with a Flicker plateau of 4×10-15 (Δν/ν=0.1) for 300 s to 103 s averaging times. These results and a preliminary study of the main effects which can induce frequency shifts are reported 相似文献
16.
Jinquan Deng Jinting Liu Shaofeng An Yongfang Tan Xiwen Zhu 《IEEE transactions on instrumentation and measurement》1994,43(4):549-552
Light shifts in a diode-laser-pumped 87Rb maser under the various conditions of laser intensities and frequency detunings were measured, and a linear dependence of the maser frequency on the laser intensities and frequencies was derived. The pulling coefficient of the maser frequency from the laser was found to be about 2.9×10-3 , and the light shift could be minimized when the laser frequency was adjusted to near the center frequency of the resonance cell 相似文献
17.
18.
提出了一种将标准短路试验波形注入多通道任意波形发生器,来产生模拟实际的校准波形,进而对测量系统进行校准的方法。校准装置使用现场可编程门阵列(FPGA)、直接数字频率合成器(DDS)等器件。对装置的检定结果表明:在10 Hz^200 kHz频率范围内,输出频率、输出电压最大误差分别为2.1×10^-6、3×10^-3。重复输出10次,输出幅值的最大相对标准偏差为5.7×10^-4,1年内幅值变化的最大相对标准偏差为1.9×10^-4。通过将该装置用于实际高压短路试验测试系统的校准,验证了试验波形的噪声、零漂及带宽均会对测量系统的准确度产生显著影响。 相似文献