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We describe the operation and performance of an optical fiber trap realized using a tapered hemispherically lensed optical fiber. Axial and transverse trapping forces exerted on a microsphere are experimentally analyzed to corroborate the optical trapping using an optical fiber. Experimental results are as follows. (i) Transverse force Ftr acting on a sphere is a restoring force that acts to pull the microsphere back to the center of trap. (ii) Axial force Fax always acts to push a sphere in the direction of the beam away from the trapping fiber end. (iii) Vector sum of Ftr and Fax acting on a sphere gives a restoring force directed back to the stable point. (iv) Transverse force Ftr plays a significant role in trapping a micro-sized object by means of an optical fiber.This paper was originally presented at the 5th International Conference on NEAR FIELD OPTICS and RELATED TECHNOLOGIES (NFO-5), which was held on December 6–10, 1998 at Coganoi Bay Hotel, Shirahama, Japan, in cooperation with the Japan Society of Applied Physics and Mombusho Grant-in Aid for Scientific Research on Priority Areas “Near-field Nano-optics” Project, sponsored by Japan Society for the Promotion of Science. 相似文献
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We have developed laser printer optics using various kinds of multiple beam generation devices, such as a polarization prism, grating, diode laser array, and optical fiber array. Recently we successfully demonstrated laser-print experiments using five beams from an optical fiber array. In the array, fibers are arranged with a spacing of 0.15 mm and emit circular Gaussian beams that have a diameter of 5 μm and a wavelength of 635 nm. The wavelength of diode lasers is determined from sensitivity of the photoconductor drum of As2Se3 material. The arrangement error vertical to the array is mostly suppressed below 0.4 μm. In the optics, curve of scan lines and print position errors in the scan direction are suppressed to a negligible size due to minimization of the magnification variation in the sub-scan direction along the print width and achromatized design, respectively.This paper was originally presented at the 2nd International Conference on Optical Design and Fabrication, ODF2000 which was held on November 15-17, 2000 at the International Conference Center, Tokyo, Waseda University, Japan. 相似文献
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在基于掺铒光纤-拉曼混合放大的可调光纤环形激光器的光纤布拉格光栅(FBG)传感系统结构基础上,提出了延长传感距离的新方法。该方法以环形掺铒光纤激光器作为光源,采用双波长拉曼放大的方法对信号进行低噪声的双向放大,系统中间的两段掺铒光纤再利用剩余的抽运功率产生自发辐射光和放大传感信号,使得整个系统能够在超长的传感距离上获得很高的信噪比。实验表明使用一只40 mW的掺铒光纤放大(EDFA)抽运源、一只170 mW的拉曼抽运源和一只2 W的拉曼抽运源,可以使整个系统的传感距离达到100km,并且传感系统的光纤布拉格光栅反射信号均能获得超过57 dB的优良信噪比,从而实现在超长距离上的光纤布拉格光栅传感。 相似文献
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YUAN Zongheng LIU Yongzhi 《Chinese Journal of Lasers》1998,7(5):390-394
1IntroductionNarowlinewidthtunablesinglefrequencysemiconductorlasersarenedforapplicationsincoherentcommunication,coherentde... 相似文献
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用光纤传输激光的方法实现激光扫描雕刻 总被引:1,自引:0,他引:1
利用扩束镜和聚焦透镜的组合,把峰值功率高达二百多千瓦的调QYAG激光耦合到光纤中,并用双透镜将光纤输出端的出射激光聚焦,成功地应用在光纤传输激光雕刻机中。 相似文献
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强反馈光纤光栅外腔半导体激光器 总被引:5,自引:0,他引:5
在理论上对强外腔反馈情形的半导体激光器线宽压窄效应进行了分析,对消反膜剩余反射率,外腔反射率,外腔腔长对线宽压缩的影响进行了研究,在实验上采用光纤光栅作为反馈元件,与一端镀有消反膜的1.5μm波段的常规多纵模交导体激光器耦合,构成强反馈光纤光栅外腔半导体激光器,得到单频窄线宽的激光输出,静态下边模抑制比大于30dB,线宽小于120kHz。 相似文献
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WANG Wenbo GAO Weijian YIN Jianping WANG Yuzhu 《Chinese Journal of Lasers》1998,7(2):108-114
TheoreticalAnalysisandExperimentalStudyonGenerationofaDarkHolowBeambyaMicron┐sizedHolowOpticalFiberWANGWenbo1,2GAOWeijian2YI... 相似文献
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Jie Liu Xiaohui Li Jiangjiang Feng Chuang Zheng Yamin Wang Aocheng Wang Xinfeng Liu 《Annalen der Physik》2020,532(3):1900454
Zinc sulfide (ZnS), which belongs to transition metal monochalcogenides, is a semiconductor material with wide direct band gap. It can potentially show some special applications (such as luminescence, phosphor, sensors, infrared window materials, photocatalysis) by changing the morphology, size, and crystal structure of semiconductor materials. However, ZnS nanospheres have not been studied as optical modulators until now. Herein, ZnS nanospheres are synthesized by the hydrothermal method and are used to realize optical modulators in an Er-doped fiber laser. The evanescent field effect is utilized to incorporate the ZnS nanospheres on a tapered fiber. Furthermore, with the increase in pump power, the modulation interval gradually decreases to a minimum of 34.36 ns corresponding to the modulation frequency of 29.1 MHz, which is the highest modulation frequency to our knowledge in a ring cavity all-fiber laser. These results demonstrate ZnS nanospheres together with the interaction of dispersion and nonlinearity in optical fibers can modulate the proposed lasers. This not only provides a new method for controlling the power and frequency of all optical modulators, but also marks an important step for ZnS materials in optics research and device applications. 相似文献
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针对目前激光分束器只能产生小发散角的问题,基于严格的非傍轴近似的衍射积分公式,提出了一种大发散角分束器的设计方法.先对目标光场分布进行坐标和光强修整,再利用改进的GerchbergSaxton迭代算法得到所需分束器的相位分布.分别采用本文设计方法和原有方法设计了发散全角为40°×40°的5×5分束器,仿真和实验结果表明:原有方法设计得到的5×5子光束存在着显著的枕形畸变,并且光强分布不均匀.而本文方法设计得到的子光束呈均匀等间隔排列,并且强度分布更为均匀. 相似文献
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数值孔径为0.07的多模光纤束与受激布里渊散位相共轭镜的组成的双光程装置中,输出光束的远场分布呈典型的二维列阵孔的径的衍射花样,输出光能分布在0.026rad内,即由单根光纤芯径的衍射极限所决定的范围内,远小于由数值孔径所决定的高阶模相应的发散范围,并且偿了由纤束不均匀性带来的缺陷。 相似文献
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A high-power singlemode Raman fiber laser (RFL) with maximum output power of 4.11 W and maximum power conversion efficiency of 47.40% at 1239 nm is realized using continuous wave 8.4 W Yb-doped double-clad fiber laser as a pump, 700 m phosphosilicate fiber, and a Raman cavity formed by a pair of fiber Bragg grating mirrors at 1239 nm. The output characteristics of the RFL at 1239 nm for different fiber lengths and output mirror reflectance are reported. Theoretical simulation is done to numerically optimize for fiber length and output coupler reflectivity to obtain maximum first Stokes power. 相似文献
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The degradation of beam quality in large-core fiber is investigated experimentally. It is found that the output beam quality factor M2 is a compound tanh function ofthe fiber lengths and misalignment launch results that the beam quality degraded faster. 相似文献
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A Brillouin fiber laser (BFL) consisting of a fiber ring resonator with different fiber temperatures emits two-frequency light output. The two-frequency BFL yields an optical beat output which can be utilized as an optical frequency shifter. The output beat frequency is controllable by the temperature difference in the fiber ring resonator and changes with a step of a resonant frequency interval of BFL. The temperature dependence of the BFL output frequency was 2.4 MHz/°C. The stability of the output beat frequency to the temperature fluctuation was estimated as 1.04°C/2.5 MHz. 相似文献
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A continuous wave (CW) high-power Raman fiber laser (RFL) with maximum output power of 2.24 W and slope efficiency of 32.8% at 1484 nm is obtained using a CW 8.4 W/ 1064 nm Yb-doped double-clad fiber laser as a pump, 700 m phosphosilicate fiber, and cascaded cavities with two pairs of fiber Bragg grating mirrors for the first and the second Stokes orders. Theoretical simulation of the RFL using a very efficient and rapidly converging collocation method is done to understand and optimize the fiber length to obtain maximum second Stokes power. RFL performance for the 300, 700 and 1150 m phosphosilicate fiber lengths was experimentally investigated by observing maximum output power, slope efficiency, threshold power, and full-width at half maximum at the second Stokes wavelength. 相似文献