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浅海温跃层声散射实验研究 总被引:1,自引:0,他引:1
本文给出1988、1989和1992年夏季南黄海海域三站位(水深34米、44米和39米)处的温跃层声脉冲反向散射实验结果。实验用窄带脉冲声源的中心频率分别为120kHz、160kHz和200kHz。实验过程中同时用CTD仪昼夜分段记录温、盐、深参数和分层拖网采集浮游生物样本。作者根据R.Kind关于平面波在任意分布不均匀层系上反射系数谱的计算方法,求出以实测温、盐垂直分布构成的不均匀层系上反射系数谱,得到跃层散射在时域上的数值模拟散射信号,与海上实测记录在时域和幅度进行对比。三年同期重复实验结果表明:实测跃层散射波到达接收点的时间与按温度剖面所做数值模拟计算结果相符。浮游生物样品分析数据与声信号记录看不出确定的对应关系,说明声散射主要是海水介质的物理不均匀性引起。 相似文献
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LD汞浦Nd:YAG激光器的连续激光输出和高重复率调Q 总被引:1,自引:1,他引:0
用连续输出1W国产多量子阱激光二极管列阵(MQW-LDA)泵浦Nd:YAG固体激光器,连续激光输出最大功率为112mW,光-光效率为10.6%,斜效率为20%,实现了连续泵浦高重复频率(1kHz,4kHz,10kHz)调Q输出,最大峰值355W,最大平均功率为43.7mW。 相似文献
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以10kHz重复率产生23W输出的小型二极管抽运激光器LishtSolutions公司的研究人员用小型二极管抽运CWNd:YAG激光器以10kHz的重复率产生出23W偏振调Q输出。这种输出具有足够高的光束质量和可以从外部有效地产生倍频的短脉宽。这种装... 相似文献
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本文报道了在较低的泵浦功率密度(10^10W/cm^2)产生光谱连续覆盖(400~870)nm,持续时间为80fs,重复频率为8kHz的高重复频率“白光”超短脉冲的实际实验系统。 相似文献
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脉冲声暴露前及暴露后即刻(1小时之内)、48小时、一周同时测试了豚鼠耳蜗畸变产物耳声发射(DPO)和振电压(CM),结果表明,暴露前豚鼠耳蜗出现最佳DPO的最适频比(f2/f1)为1.19-1.25,最适强度差(If1-If2)为0.45—2.00dB,8和4kHz时DPO出现率为100%,2kHz为95%,1kHz时为79%。暴露后不同阶段DPO和CM恢复的速率和变化程度不同,前者在各个阶段上损失的程度比后者重。震后一周DPO除在8kHz时恢复至接近震前水平外,其余频率只恢复至震前的1/4左右或稍多.与之对比,各个频率的CM在一周时均完全恢复至震前水平,似说明DPO较CM敏感。DPO和CM相关分析结果提示,二者同源于外毛细胞(OHC). 相似文献
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数值模拟二维间隙表面等离子波导传输特性 总被引:2,自引:2,他引:0
利用表面等离子激元的新颖特性,设计了二维间隙表面等离子波导.以这种结构为基础通过变形和组合形成90°直角弯曲波导、T型光功率分配器和光开光,采用时域有限差分法研究了它们的传输特性.结果表明:不同于介质光波导的弯曲损耗来自于辐射泄漏,90°直角弯曲间隙表面等离子波导的能量损耗主要来自于金属中的欧姆热损耗.在间隙达到40 nm以上后,当直行段的长度适当时,弯曲段的透射率较相同长度的直波导的透射率要大.T型光功率分配器在两输出波导的间隙宽度比达到0.6及以上时,不同于传统介质波导的分光原则,能量主要沿等效折射率较小的输出臂流出.当两输入光的相位反相时,T型光开关处于输出截止的状态,当两输入光的相位同相时,T型光开关处于输出导通的状态.所有波导间隙均小于衍射极限,实现了超衍射极限传播,可用于未来了超大规模集成光路中. 相似文献
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相比于传统的1×N对称型多模干涉(Mult-Mode Interference,MMI)分束器设计,提出了一种新型埋入式弱限制光波导分束器件.它的干涉区及输入输出波导采用倒锥形式,器件尺寸减小,且不均匀性与附加损耗也减小.以1×4的对称型MMI分束器为例,当只对干涉区采用倒锥形结构后,在TE偏振中心波长为1.55 μm时,器件长度减小了500 μm,均匀性增加了0.131 dB,而附加损耗仅增加了0.02 dB,波长响应较传统设计增加了40 nm.在此基础上,又在输入输出臂上也各增加倒锥形结构后,相比于传统设计附加损耗减小了0.02 dB,均匀性增加了0.139 dB,器件长度减小了500 μm.改进后的器件具有优越的容差性.器件采用掺氟型聚合物材料进行优化设计,通过在合理范围内偏离输出波导位置,使输出光强达到最大值. 相似文献
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A compact multimode interference (MMI) splitter with silicon photonic nanowires on silicon-on-insulator (SOI) substrate is designed and fabricated. The footprint of the MMI section is only approximately 3×10 (μm). The simulation results show that the device may have a low excess loss of 0.04 dB. The transmission loss of the silicon photonics wire is measured to be 0.73±0.3 dB/mm. The compact size and low transmission loss allow the device to be used in ultra-compact photonic integrated circuits. The device exhibits a good light splitting function. In a spectral range of 1549-1560 nm, the excess loss is 1.5 dB and the average imbalance between the two channels is 0.51 dB. 相似文献
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《Photonics and Nanostructures》2014,12(2):184-188
We propose a design of a low loss terahertz polarization splitter based on a dual-core terahertz fiber with crossed dielectric strips in the fiber cross section. Low transmission loss is realized by extending the mode field to the air holes adjacent to the solid material. An 11.4-cm-long terahertz polarization splitter is obtained with the extinction ratio better than −15 dB and a bandwidth of 16 μm. 相似文献
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The equivalent singularity method is developed for the analysis of sound propagation in a duct with a thin solid or point-reacting porous splitter of a finite streamwise length. The method consists in representing the splitter by a singular plane of pressure dipoles and mass sources, distributions of which are determined so that the boundary condition at the splitter surfaces is satisfied. The boundary condition is expressed in terms of two admittance parameters giving relations between pressures and normal displacements of fluid particles at the upper and lower surfaces of the splitter. Computed results are presented to illustrate the dependence of the sound power transmitted through the splitter section on the acoustic properties, length and location of the splitter and the flow Mach number. A principal cause of the sound attenuation due to a splitter is found to be the conversion of the acoustic energy into the wake vortex energy convected downstream. A solid splitter or a porous splitter of small admittance shows tuning effects—with a peak or multiple peaks in the attenuation spectrum. The tuning frequencies can be controlled by the splitter location. 相似文献
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R. An Y. Li D. Liu Y. Dou F. Qi H. Yang Q. Gong 《Applied Physics A: Materials Science & Processing》2007,86(3):343-346
We investigated the femtosecond laser writing of optical waveguides inside Foturan glass at various pulse energies and focusing
depths. An optimal waveguide fabricated solely by femtosecond laser irradiation showed a refractive index modulation of ∼1.7×10-3 and a minimum transmission loss of ∼0.80 dB/cm. This type of waveguide had lower transmission loss than those fabricated
by a hybrid process of femtosecond laser exposure and following thermal treatment. An optical splitter was also fabricated
at high pulse energy.
PACS 42.65.Re; 42.82.Et; 42.70.Gi 相似文献
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Chao Dou Xili Jing Shuguang Li Junjun Wu Qingbo Wang 《Optical and Quantum Electronics》2018,50(6):255
The characteristics of a novel dual-core photonic crystal fiber are investigated. In the center of photonic crystal fiber, an energy transmission channel is introduced. The optimized photonic crystal fiber can be used for polarization splitter, which has a short length and low loss. 相似文献