61 resultados para Prati, Alessio, 1750-1788.
em Chinese Academy of Sciences Institutional Repositories Grid Portal
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IEECAS SKLLQG
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在对涡激振动圆柱的附加质量进行理论分析的基础上,综合实验和数值模拟的结果,根据涡激振动中结构振动频率、来流约化速度的关系,推导出涡激振动锁频阶段的圆柱附加质量系数估算公式。通过对有关圆柱涡激振动实验结果和数值模拟结果进行分析,并与有关圆柱涡激振动实验结果进行对比,表明本文提出的圆柱涡激振动锁频阶段附加质量系数的估算公式与实验结果是相吻合的。另外,本文还以单自由度弹簧质量阻尼模型为研究对象,在对其涡激振动中的附加质量进行理论分析的基础上,给出了上述估算公式的适用条件。最后,做为应用算例,考察比较了进行附加质量修正和不修正两种情况下的圆柱涡激振动响应。结果表明采用本文提出的附加质量计算公式,能够更好地预测涡。
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利用低维Galerkin方法及Floquet稳定性分析理论,计算分析了圆柱绕流的三维线性不稳定性.分析中构造了能较好描述尾迹区流动的周向基函数,建立了完备的合理的基函数组,改进了计算机算法.结果证实圆柱二维周期流对展向小扰动为不稳定的,正确地预计了出现三维长波不稳定性的临界雷诺数Re_c=190,扰动展向波长为λ_c=3.6d.对雷诺数Re为180,190两种工况下的圆柱三维绕流流场的计算进一步证实了这种流动的整体不稳定性.该文所预计的临界值比Noack等人的结果更为精确,与Barkley等人的DNS解一致,与Williamson的实验相符.
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Based on the Mach-Zehnder effect between the core mode and the cladding modes, the interference fringes are formed by a pair of cascaded long-period fiber gratings (CLPFGs). Theoretical analyses show that the spectral spacing and the wavelength of these fringes are functions of the waveguide dispersion factor gamma, which is a characterizing parameter to LPFG and with theoretical and applicational significance. By measuring the characteristics of the transmission spectra of CLPFGs, the absolute value of gamma can be obtained. At the same time, the thermo-optic coefficient of effective refractive index difference between core and cladding modes, p, can also be obtained by measured the temperature sensitivity of these fringes. In the experiments, \gamma\ and mu were measured by this method to be 0.874 and 4.08 x 10(-5) degreesC(-1), respectively, for LPFGs with period of 450 mum and with a HE14 resonant peak at 1554 nm. (C) 2004 Elsevier B.V. All rights reserved.
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提出了一种在双掺杂铌酸锂晶体中用调制的双紫外光进行非挥发全息记录的方法。与通常的用紫外光敏化的非挥发全息记录相比,这种方法可以大幅度地提高光栅强度和记录灵敏度。联立双中心物质方程和双光束耦合波方程,数值分析了光栅强度和衍射效率随时间的变化并讨论了掺杂浓度和记录光强对紫外光非挥发全息记录机制下光折变效应的影响。研究发现,紫外光记录得到的深浅中心的光栅具有相同的相位,总的光栅(深浅中心光栅的叠加)强度为两光栅强度之和,固定过程中深中心的光栅得到增强;增大深浅中心掺杂的浓度可以提高光栅强度,增大记录紫外光的光强
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SrBi2Ta2O9 (SBT) thin films on quartz substrates were prepared by use of the pulsed-laser deposition technique. The nonlinear refractive indices, n(2), Of the SBT films were measured by use of z-scan techniques with picosecond pulses. Large negative nonlinear refractive indices of 3.84 and 3.58 cm(2)/GW were obtained for the wavelengths 532 nm and 1.064 mum, respectively. The two-photon absorption coefficient was determined to be 7.3 cm/GW for 532 nm. The limiting behavior of SBT thin film on a quartz substrate was investigated in an f/5 defocusing geometry by use of 38-ps-duration, 532-nm, 1.064-mum. laser excitation. (C) 2001 Optical Society of America.
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采用燃烧法制备了Nd:YSAG粉体,经过成型、素烧,最终在氢气气氛中烧结制备了Nd:YSAG透明陶瓷.测试结果表明,Nd:YSAG透明陶瓷具有荧光谱线较宽,荧光寿命较长的特点.激光实验得到的激光输出,斜率效率为23.6%,输出功率为0.36W,输出激光的谱线分布较宽.
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采用传统无压烧结工艺在氢气氛下制备Al2O3透明陶瓷。实验结果表明:MgO和La2O3复合添加时,随着La2O3掺杂量的增加体积密度总体上保持上升的趋势。随着保温时间的延长,陶瓷的致密化程度增大,残余气孔逐步排出,晶粒进一步长大。采用La2O3和MgO复合添加比单独掺入MgO陶瓷样品透过率更高,掺杂效果更好。在烧结温度为1750℃,保温时问为1h条件下,在波艮为300~800nm测试范围内,陶瓷样品的全透过率大于82%,最大值为86%。
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Transparent polycrystalline Nd:YAG ceramics were fabricated by solid-state reactive sintering a mixture of commercial Al2O3,Y2O3, and Nd2O3 powders. The powders were mixed in ethanol and doped with 0.5 wt% tetraethoxysilane, dried, and pressed. Pressed samples were sintered at 1750 degrees C in vacuum. Transparent fully dense samples with average grain sizes of 10 mu m were obtained. The 1 at.% Nd:YAG ceramic was used to research passively Q-switched laser output with a Cr4+:YAG crystal as a saturable absorber. An average output power of 94 mW with a pulse width of 50 ns was obtained when the incident pump power was 750 mW. The slope efficiency was 13%. The pulse energy is 5 mu J, and the peak power is about 100 W.
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LaF3 thin films were prepared by thermal boat evaporation at different substrate temperatures and various deposition rates. X-ray diffraction (XRD), Lambda 900 spectrophotometer and X-ray photoelectron spectroscopy (XPS) were employed to study crystal structure, transmittance and chemical composition of the coatings, respectively. Laser-induce damage threshold (LIDT) was determined by a tripled Nd:YAG laser system with a pulse width of 8 ns. It is found that the crystal structure became more perfect and the refractive index increased gradually with the temperature rising. The LIDT was comparatively high at high temperature. In the other hand, the crystallization status also became better and the refractive index increased when the deposition rate enhanced at a low level. If the rate was super rapid, the crystallization worsened instead and the refractive index would lessen greatly. On the whole, the LIDT decreased with increasing rate. (C) 2007 Elsevier B.V. All rights reserved.