343 resultados para PDMS fiber


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低损耗实芯碲酸盐光纤的非线性研究

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微全分析系统是目前很前沿的研究领域,尽管现在还没有真正意义的微全分析系统出现,但它代表了分析科学的发展趋势。本文主要研究了ITO导电玻璃和PDMS微芯片毛细管电泳和电化学发光检测方法。微芯片毛细管电泳对与其联用的检测器有相当高的要求,一些传统的检测方法很难适应于微芯片毛细管电泳。电化学发光检测是一种新兴的检测技术,在化学、生物、医学诊断以及免疫分析中展现出良好的应用前景。如何实现和完善微芯片毛细管电泳与电化学发光检测联用技术是本论文的重点。我们采用聚二甲基硅氧烷(poly(dimethylsiloxone),简称PDMS)和玻璃作为芯片材料,以锢锡氧化物(indium桩n oXide,简称工T0)导电玻璃为工作电极设计了一种集成化的微芯片毛细管电泳电化学发光检测器。其中,芯片的底片由工TO导电玻璃经光刻、化学腐蚀等方法处理后得到。ITO是一种透明的导电材料,作为工作电极集成到芯片的底片上,PDMS层与芯片底片采用可逆键合的方式键合,大大简化了操作并提高了电化学发光信号的采集效率。我们采用脯氨酸作为被测物对检测器进行了表征。在实验过程中,微芯片毛细管电泳及工T0工作电极都表现出良好的稳定性。我们还提出了电化学和电化学发光同时检测技术,应用于微芯片毛细管电泳和常规毛细管电泳。在这种电化学和电化学发光双检测模式中,三联吡陡钉(Ru(bpy)32+既作为电化学发光检测所需的发光试剂与被分析物反应生成激发态的Ru(bpy)32+*产生电化学发光信号,又在电极表面平行催化电化学反应得到增强的电流响应,提高电化学检测的灵敏度。电化学信号与电化学发光信号同时产生并分别记录,从而实现了电化学和电化学发光同时检测。我们将这种检测技术与芯片或常规毛细管电泳结合,以多巴胺及三种药物分子山蓖若碱、氧氟沙星和利多卡因作为被测物对其进行了表征。这种同时检测方法与其它多检测模式相比更为简单、方便,比单一的电化学或电化学发光检测可以获得更多的被分析物信息,扩大单一检测方式的应用范围。

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The use of alpha-power chirped fiber Bragg gratings for dispersion cancellation in an optical fiber link is discussed. Numerical and theoretical investigation of recompressing the dispersion-broadened pulse by using alpha-power chirped gratings is made, which shows that, the dispersion-broadened Gaussian pulse after 100 km standard fiber (with zero dispersion at lambda = 1.3 mu m) trnasmission at lambda = 1.55 mu m with initial width of T-FWHM = 33ps (full width at half maximum) can be perfectly recompressed with the peak reflectivity of 82% by using a 30 mm long alpha-power chirped fiber grating with proper a value and optimal grating parameters.

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We propose a fiber-to-waveguide coupler for side-illuminated p-i-n photodiodes to obtain high responsivity and low polarization dependence that is grown on InP substrate and is suitable for surface hybrid integration in low cost modules. The fiber-to-waveguide coupler is based on a diluted waveguide,which is composed of ten periods of undoped 120nm InP/80nm InGaAsP (1.05μm bandgap) multiple layers. Using the semi-vectorial three dimensional beam propagation method (BPM) with the central difference scheme,the coupling efficiency of fiber-to-waveguide under different conditions is simulated and studied,and the optimized conditions for fiber-to-waveguide coupling are obtained. For TE-like and TM-like modes,the calculated maximum coupling efficiency is higher than 94% and 92% ,respectively. The calculated polarization dependence is less than 0. ldB,showing good polarization independence.

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A fiber coupled module is fabricated with integrating the emitting light from four laser diode bars into multimode fiber bundle. The continuous wave (CW) output power of the module is about 130 W with a coupling efficiency of around 80%. The output power is very stable after the temperature cycling and vibration test. No apparent power decrease has been observed as the device working continuously for 500 h.

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A polarization-maintaining (PM) fiber Mach-Zehnder (MZ) interferometer has been established to measure the EO effect of very thin film materials with optical anisotropy. Unlike a common MZ interferometer,all the components are connected via polarization-maintaining fibers. At the same time, a polarized DFB laser with a maximum power output of 10mW is adopted as the light source to induce a large extinction ratio. Here, we take it to determine the electro-optical coefficients of a very thin superlattice structure with GaAs, KTP, and GaN as comparative samples. The measured EO coefficients show good comparability with the others.

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A cladding-pumped ytterbium-doped fiber laser is described in this letter. Using unusual pumping source with 915-nm wavelength, slope efficiency up to 75% with respect to absorbed input power and output power is obtained, a maximum output power of 4.006 W with fundamental mode is measured.

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The butt-coupling between a semiconductor laser diode and a fiber Bragg grating external cavity acts a key roll on the laser characteristics. The scatter matrix method considering the butt-coupling efficiency is used to analyze the butt-coupling between them. It is found that the butt-coupling distance and coupling efficiency determine the laser characteristics. For strong feedback, the single lasing wavelength changes in the reflection bandwidth of the effective reflectivity ( approximately the Bragg region of the fiber Bragg grating) as the distances change. For weak feedback condition, some different results are obtained. The SMSRs in the two conditions are presented and analyzed. These results can provide important design guidance of device parameters for the practical fabrication.

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The theoretical investigation of the coupling efficiency of a laser diode to a single mode fiber via a hemispherical lens on the tip of the tapered fiber in the presence of possible transverse offset and angular mismatch is reported.Without the misalignment,coupling efficiency increases with the decreasing of taper length.With the misalignment,this relation is that the coupling efficiency decreases with each kind of offset.

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Based on a set of microoptics the output radiation from a continuous wave (CW) linear laser diode array is coupled into a multi-mode optical fiber of 400 ptm diameter. The CW linear laser diode array is a 1 cm laser diode bar with 19 stripes with 100 fxm aperture spaced on 500 (xm centers. The coupling system contains packaged laser diode bar, fast axis collimator, slow axis collimation array, beam transformation system and focusing system. The high brightness, high power density and single fiber output of a laser diode bar is achieved. The coupling efficiency is 65% and the power density is up to 1.03 * 10~4 W/cm~2.

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A piece of multimode optical fiber with a low numerical aperture (NA) is used as an inexpensive microlens to collimate the output radiation of a laser diode bar in the high numerical aperture (NA) direction. The emissions of the laser diode bar are coupled into multimode fiber array. The radiation from individual ones of emitter regions is optically coupled into individual ones of fiber array. Total coupling efficiency and fiber output power are 75% and 15W, respectively.