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131.
内壁蜂窝结构是决定遮光罩杂散光抑制性能的主要因素,掌握其各向异性辐射传输特性对遮光罩的杂散光分析和优化设计具有重要意义.针对蜂窝结构单元,建立辐射传输模型,导出了表面双向反射分布函数的离散表达式;通过蒙特卡罗法模拟蜂窝结构单元的辐射传输过程,分析了几何参量和涂层反射率对等效面反射特性的影响;根据模拟所得双向反射分布函数数据库,建立了用于遮光罩杂散光分析的蜂窝结构等效面的反射特性概率模型.分析结果表明,蜂窝结构对杂散光呈现很强的后向散射特征,等效面的反射特性概率模型与直接模拟结果符合很好,可用于遮光罩杂散光分析和设计. 相似文献
132.
133.
�� ����������������ʤ���� ������ �죬���¶������ع� 《核聚变与等离子体物理》2015,35(4):373-378
Different ratios of methane/air in the low power arc discharges assisted methane combustion were studied at atmospheric pressure. Plasma emission spectroscopy was recorded by an optical emission spectrometer. The possible physical and chemical reaction process and mechanisms were discussed. With a plasma in the on or off state, the physical appearances of the methane combustion flame were observed and compared, the temperature of the flame in the main combustion zone was investigated. The gas compositions of CH4, CO and O2 were analyzed by the gas chromatography and flue gas analyzer. The results showed that when plasma was in the on state, the temperature of flame increased and the combustion efficiency enhanced in stable combustion due to decrease of CH4, CO and O2; the combustion enhancement was more obvious at low ratio of methane/air; the rich combustion limits in terms of the ratio of methane/air was extended from 16% to 21%. 相似文献
134.
135.
为解决点源法计算全息速度较慢的问题,提出了一种新的查表算法,命名为三角函数查表法(T-LUT算法)。该算法是基于点源法基本的数学公式,通过一系列数学近似与恒等变换,生成了一种纯相位查找表,该查找表具有三维特性,并具有生成速度快、精度高、占用内存少等特点,克服了点源法重复计算相位的缺点。同时采用统一计算设备架构(CUDA)并行计算在图形处理器(GPU)上加以实现,并进行了三次并行优化。在算法的验证与对比实验中,采用单显卡(GPU显卡)实现T-LUT算法,在不牺牲全息图再现像质量的前提下,成功地将点源法计算全息的速度大幅度提升。实验发现在不同的物空间采样点数量的情况下,速度相对于点源法GPU运算提升30倍至近千倍不等。 相似文献
136.
QIN Qing HUANG Nan LIU Wei-Bin LIU Yu-Dong PENG Yue-Mei QIU Jing WANG Dou WANG Xin-Hao WANG Na WANG Jiu-Qing WEI Yuan-Yuan WEN Xue-Mei XING Jun XU Gang Yu Cheng-Hui ZHANG Chuang ZHANG Yuan ZHAO Zheng ZHOU De-Min 《中国物理C(英文版)》2009,33(Z2)
During the 1st and 2nd stages of the commissioning of the upgrade project of the Beijing Electron Positron Collider(BEPC Ⅱ),which started on Nov.12,2006 and Oct.24,2007,respectively,we got the luminosity one tenth of its design value,provided beams to synchrotron radiation users for about 4 months,and studied beam dynamics as well.In this paper,some beam dynamics studies on the storage rings and their preliminary results are given. 相似文献
137.
Qian W Chuang SC Amador RB Jarrosson T Sander M Pieniazek S Khan SI Rubin Y 《Journal of the American Chemical Society》2003,125(8):2066-2067
A rational synthetic approach to the first four-membered ring-containing derivatives of C(62) is reported. They were synthesized by an inverse electron demand Diels-Alder reaction of 3,6-diaryl-1,2,4,5-tetrazines with C(60) in o-dichlorobenzene, followed by visible light irradiation at reflux. The structure of these nonclassical fullerenes derivatives was determined by X-ray single-crystal diffraction. 相似文献
138.
Steffen M Vandersypen LM Chuang IL 《Journal of magnetic resonance (San Diego, Calif. : 1997)》2000,146(2):369-374
The rotation of a spin subject to an on-resonance soft pulse and simultaneously to a soft pulse at a nearby frequency may strongly deviate from the desired rotation expected for a single on-resonance pulse. The deviation is the result of transient frequency shifts of the spin caused by the off-resonance irradiation. We show that the resulting error can be corrected by shifting the frequency of the on-resonance pulse in such a way that it tracks the shift of the spin frequency. Experimentally, the effectiveness of this simple and intuitive method is demonstrated for simultaneous inversions at nearby frequencies in the case of both coupled and uncoupled spins. Simulations predict that the correction technique is effective for arbitrary pulse shapes and tip angles and is particularly useful when the frequency window of the shaped pulse is two to eight times the frequency separation between the chemical shifts of the two spins. 相似文献
139.
Hai-Han Lu Shah-Jye Tzeng Yao-Wei Chuang Guan-Lin Chen Hsiang-Chun Peng 《Optics Communications》2007,271(2):436-440
A directly-modulated amplitude modulation-vestigial sideband (AM-VSB) cable television (CATV) erbium-doped fiber amplifier (EDFA)-repeated system that uses split-band technique and photonic crystal fiber (PCF) as a broadband dispersion compensation device is proposed and demonstrated. In contrast to a conventional externally-modulated fiber-optic CATV system, good performance of carrier-to-noise ratio (CNR), composite second order (CSO) and composite triple beat (CTB) were obtained in our proposed systems over a combination of 100-km single-mode fiber (SMF) and 3.6 km PCF. 相似文献
140.
Chuang WT Hsieh CC Lai CH Lai CH Shih CW Chen KY Hung WY Hsu YH Chou PT 《The Journal of organic chemistry》2011,76(20):8189-8202
o-Hydroxy analogues, 1a-g, of the green fluorescent protein chromophore have been synthesized. Their structures and electronic properties were investigated by X-ray single-crystal analyses, electrochemistry, and luminescence properties. In solid and nonpolar solvents 1a-g exist mainly as Z conformers that possess a seven-membered-ring hydrogen bond and undergo excited-state intramolecular proton transfer (ESIPT) reactions, resulting in a proton-transfer tautomer emission. Fluorescence upconversion dynamics have revealed a coherent type of ESIPT, followed by a fast vibrational/solvent relaxation (<1 ps) to a twisted (regarding exo-C(5)-C(4)-C(3) bonds) conformation, from which a fast population decay of a few to several tens of picoseconds was resolved in cyclohexane. Accordingly, the proton-transfer tautomer emission intensity is moderate (0.08 in 1e) to weak (~10(-4) in 1a) in cyclohexane. The stronger intramolecular hydrogen bonding in 1g suppresses the rotation of the aryl-alkene bond, resulting in a high yield of tautomer emission (Φ(f) ≈ 0.2). In the solid state, due to the inhibition of exo-C(5)-C(4)-C(3) rotation, intense tautomer emission with a quantum yield of 0.1-0.9 was obtained for 1a-g. Depending on the electronic donor or acceptor strength of the substituent in either the HOMO or LUMO site, a broad tuning range of the emission from 560 (1g) to 670 nm (1a) has been achieved. 相似文献