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 共查询到19条相似文献,搜索用时 593 毫秒
1.
李也凡 《发光学报》1998,19(4):352-356
为准确探测射频信号中所携带的全部信息,包括信号的幅度,频率和相位等,并有效地增加探测系统的动态范围,采用信道化体皮声光外差探测方法,这里给出这种体声光外左接收机的基本原理,光路设计的基本方法以及实验样机的测试结果。  相似文献   

2.
空间积分声相关处理的研究   总被引:1,自引:0,他引:1  
何大伟  许承杰 《光学学报》2000,20(11):514-1517
利用声光布拉格器件成功地设计并研制出了空间积分声光相关器,实现了对模拟雷达信号(占空比为50%,重复频率1MHz,载频为140MHz)的空间积分声光相关检测。  相似文献   

3.
生卫东  刘宏伟 《光学学报》1995,15(9):195-1198
报道了用两个1.5W激光二极管偏振耦合端面泵浦的声光调Q内腔倍频Nd:YAG激光器。输出532nm绿光重复频率1KHz时,最大峰值功率为2.23KW,最窄脉宽为18ns,平均功率40mW。最高重复频率30KHz。重复频率15kHZ时,最高平均率128mW。对声光调Q内倍频Nd:YAG激光器的动态特性进行了理论分析及计算。  相似文献   

4.
王骐  田兆硕 《光学学报》2000,20(11):473-1476
报道了采用不等长电极结构的射频激励双通道波导CO2激光器,通过调节射频电源功率的方法可以调谐双通道输出激光的外差频率,其调谐率约为0.1MHz/W。在未采取任何措施时,其短期外差频率稳定性可达10^-10。还在理论上分析了射频功率调谐外差频率的原理。  相似文献   

5.
1.319μm连续固体锁模激光器   总被引:3,自引:0,他引:3  
陈越峰  张世文 《光学学报》1994,14(4):69-371
报道了1.319μmNd:YAG连续锁模激光器的技术研究。激光器的谐振腔为低热敏腔,用声光振幅调制器作为锁模元件,泵浦腔具有较高的泵浦效率和输出稳定性,获得了重复频率100MHz,平均功率~0.54W,脉宽<170ps的光脉冲。  相似文献   

6.
集成光学声光可调谐波长滤波器的研制   总被引:13,自引:2,他引:11  
薛挺  祁芳  胡鸿璋  丁荣林  耿凡 《光学学报》2000,20(8):095-1099
阐述了中心波长为1.523μm的集成光学声光可调谐波长滤波器的各项理论参数、制作工艺以及性能测试。在有效声光相互作用长度16mm、射频驱动功率35mW时,获得了模式转换效率大于99%、插入损耗小于-4.dB、带宽1.6nm、3dB调谐范围为140nm的实验结果。  相似文献   

7.
双KTP内腔参量下转换产生量子相关孪生光子对   总被引:5,自引:2,他引:3  
王海  薛晨阳 《光学学报》1997,17(8):002-1005
使用双KTP晶体串接,经光学参量振荡腔内参量下转换,在300mW泵浦功率下,获得总功率约23mW的强度相关的孪生光束,在1.25MHz处其强度差噪声功率较散离噪声极限降低50%(3dB)。  相似文献   

8.
廖欣  何宁  陈明  陈名松 《光学学报》2008,28(s2):278-282
为使现代电子侦察技术能适应信号密集、宽频谱、大动态的电磁环境, 提出了一种基于声光偏转器实现相关光信号处理的方法, 分析了射频信号频率变化与布拉格衍射角的关系, 讨论了声光偏转效应对信号频率的空间滤波特性; 在理论分析的基础上, 构建了在可见光范围内实现声光偏转的相干光信号探测的实验系统, 并通过计算机仿真对比, 验证了这种方法的可行性。实验表明, 采用波长为630 nm的单频激光, 带宽为200 MHz的声光偏转器, 其频率分辨率优于1 MHz, 频率信号的空间分离效果明显, 接收灵敏度和信噪比得到改善。  相似文献   

9.
单频运转的Nd:YVO4激光器   总被引:5,自引:2,他引:3  
林岳明  何慧娟 《光学学报》1995,15(3):71-373
报道了激光二极管纵向泵浦单频运转的Nd:YVO4激光器,用波长为809nm激光二极管的连续输出功率660mW泵浦,获得1064nm,功率为155mW连续单频输出,泵浦阈值226mW,斜率效率33.8%,线宽小于10MHz.  相似文献   

10.
傅焰峰  李涛 《光学学报》1997,17(8):113-1116
对1.5μm波导型声光TE-TM模式转换光滤波器进行了研究。采用了可降低驱动功率的表面声波导结构。在1.5 ̄1.6μm波段实现了可调滤光,通带宽度小于2nm,达到97¥以上转换率所需的射频驱动功率约80mW(19dBm),器件总插入损耗约9dB。  相似文献   

11.
A new type of optical fiber hydrophone is constructed with a fiber Bragg grating (FBG) based on the intensity modulation of laser light in an FBG under the influence of sound pressure. The FBG hydrophone shows linearity, with dynamic range about 70 dB. It can measure amplitude and phase of an acoustic field in real time, and operates in a wide range of acoustic frequency, at least from 1 kHz to 3 MHz. No signal distortion is observed in the detected signal. Because of the simplicity in its operating principle and geometry, an FBG hydrophone is expected to be an acoustic sensor of high practicality compared to a conventional optical fiber hydrophone.  相似文献   

12.
We present a pump-and-signal-resonant optical parametric oscillator that provides 25 dB of amplitude noise suppression of the transmitted pump beam from dc to 20 kHz. The upper frequency range of the optical limiter increases as the pump power is increased, up to 1 MHz with 580 mW of input power. The amount of noise suppression is limited by pump-depletion effects. The upper frequency range is limited by the temporal response of the device. We present a numerical analysis that predicts this behavior.  相似文献   

13.
We have proposed and demonstrated a double-pass ytterbium-doped fiber amplifier using an optical circulator and a fiber Bragg grating as reflector. When the signal has passed through the ytterbium-doped fiber once, it reflects off a 0.2-nm passive fiber Bragg grating filter. This reduces amplified spontaneous emission (ASE) noise from the first pass. The input signal light is amplified both forward and backward through ytterbium-doped fiber. With this double-pass configuration, 1053.15-nm unsaturated signal gain of 28 dB, gain coefficient of 1.1 dB/mW, and noise figure of less than 4 dB are achieved at 977-nm pump power of 68 mW. It is also found that this double-pass configure provides enhancing gain coefficient and improving noise figure by comparison with single-pass configuration.  相似文献   

14.
Very little is known about the blood backscattering behavior and signal statistics following flow stoppage at frequencies higher than 10 MHz. Measurements of the radio frequency (rf) signals backscattered by normal human blood (hematocrit = 40%, temperature = 37 degrees C) were performed in a tube flow model at mean frequencies varying between 10 and 58 MHz. The range of increase of the backscattered power during red blood cell (RBC) rouleau formation was close to 15 dB at 10 and 36 MHz, and dropped, for the same blood samples, below 8 dB at 58 MHz. Increasing the frequency from 10 to 58 MHz raised the slope of the power changes at the beginning of the kinetics of aggregation, and could emphasize the non-Gaussian behavior of the rf signals interpreted in terms of the K and Nakagami statistical models. At 36 and 58 MHz, significant increases of the kurtosis coefficient, and significant reductions of the Nakagami parameter were noted during the first 30 s of flow stoppage. In conclusion, increasing the transducer frequency reduced the magnitude of the backscattered power changes attributed to the phenomenon of RBC aggregation, but improved the detection of rapid growth in aggregate sizes and non-Gaussian statistical behavior.  相似文献   

15.
Underwater Acoustic Sensor with Fiber Bragg Grating   总被引:1,自引:0,他引:1  
A new type of underwater acoustic sensor is proposed with an optical fiber Bragg grating (FBG). Because of the photoelasticity with respect to the refractive index and the elasticity of the fiber, the sound pressure in water modulates the Bragg reflection wavelength and, in turn, the intensity of the laser light transmitted through the FBG fiber. Good linearity between the detected signal and the sound pressure is obtained in the range from 81 dB to 140 dB re 1 μPa. Since the upper and lower limits of the acoustic signal level for operation of the sensor are limited by the driving circuit and the transduction of the sound in water, the sensor is expected to operate with much larger dynamic range both at higher and lower pressure levels. Operation of the sensor is very stable with the insertion of optical isolators into the system, although without the isolators the output signal fluctuates at low frequency due to the Fabry-Perot interference effect between the FBG and the various facets.  相似文献   

16.
We describe and demonstrate a novel technique for continuously tuning the frequency of a dual-loop-configuration optoelectronic rf oscillator. The rf tunability is obtained from a tunable diode laser and dispersive optical fibers. Results are presented for three ranges of frequency, centered at 550 MHz, 3 GHz, and 9 GHz. The frequency can be tuned electrically with constant rf power within a range of 0.1-1.9 MHz, depending on the center oscillation frequency. The tuning range can be increased eightfold through the use of highly dispersive fibers.  相似文献   

17.
本文利用周期极化磷酸氧钛钾晶体构成的半整块结构简并光学参量振荡器实验制备了连续变量光通信波段低频压缩态光场。光学参量振荡器的阈值功率为210 mW。当775nm抽运光场功率为130 mW时,在分析频段50kHz~900kHz范围内获得真空压缩态光场。在200kHz分析频率处,压缩态光场的最大压缩度达5.0dB;在最低分析频率50kHz处,压缩态光场的压缩度为2.0dB。该低频压缩态光场可为基于光纤的量子精密测量提供量子光源。  相似文献   

18.
在热压缩态中测量相位算符的涨落   总被引:1,自引:1,他引:0  
董传华 《光学学报》1997,17(8):97-1001
利用热场动力学的方法计算了热压缩态中测量相位算符的涨落,引入了两种类型的基础量子涨落,一种是与测量相位的两个正交分量相联系,另一种是与一个测量相位分量和光子数相联系。由此,研究了热压缩压中测量相位涨落的两种压缩及其与温度的关系。  相似文献   

19.
We present experimental results for what is to our knowledge the first spectral-hole-burning based rf spectrum analyzer to cover 10 GHz of rf analysis bandwidth. The rf signal of interest is modulated onto an optical carrier, and the resultant optical sidebands are burned into the inhomogeneously broadened absorption band of a Tm3+:YAG crystal. At the same time a second, frequency-swept laser reads out the absorption profile, which is a double-sideband replica of the rf spectrum, and thus the rf spectrum can be deduced after spectral calibration of the nonlinear readout chirp. This initial demonstration shows spectral analysis covering 10 GHz of bandwidth with >5500 spectral channels and provides 43 dB of dynamic range.  相似文献   

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