Jiang Junfeng
Tianjin University
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Publication
Featured researches published by Jiang Junfeng.
Frontiers of Electrical and Electronic Engineering in China | 2006
Jiang Junfeng; Lin Tie-gen; Zhang Yimo; Li Chuan; Sun Jie; Ding Sheng
The Talbot interferometer used for writing fiber Bragg grating (FBG) is analyzed effectively in this paper. Based on electromagnetic theory, a computing model of the Talbot interferometer is established with the temporal and the spatial coherence taken into account and with the turning angle of the reflectors as a critical parameter. The model can provide a more detailed and precise information about the interference field and is used to study the effect of the turning error of the reflectors in writing FBG. The calculation result shows that the turning error has an important effect on the visibility of the far interference field.
2017 International Conference on Optical Instruments and Technology: Optoelectronic Imaging/Spectroscopy and Signal Processing Technology | 2018
Zhang Yongning; Jiang Junfeng; Liu Kun; Huang Can; Wang Shuang; Zhang Xuezhi; Liu Tiegen; Guohai Situ; Liquan Dong; Xun Cao; Wolfgang Osten
Coherent Anti-Stokes Raman Scattering (CARS) microscopy has attracted lots of attention because of the advantages, such as noninvasive, label-free, chemical specificity, intrinsic three-dimension spatial resolution and so on. However, the temporal overlap of pump and Stokes has not been solved owing to the ultrafast optical pulse used in CARS microscopy. We combine interference spectrum of residual pump in Stokes path and nonlinear Schrodinger equation (NLSE) to realize the temporal overlap of pump pulse and Stokes pulse. At first, based on the interference spectrum of pump pulse and residual pump in Stokes path, the optical delay is defined when optical path difference between pump path and Stokes path is zero. Then the relative optical delay between Stokes pulse and residual pump in PCF can be calculated by NLSE. According to the spectrum interference and NLSE, temporal overlap of pump pulse and Stokes pulse will be realized easily and the imaging speed will be improved in CARS microscopy.Coherent Anti-Stokes Raman Scattering (CARS) microscopy has attracted lots of attention because of the advantages, such as noninvasive, label-free, chemical specificity, intrinsic three-dimension spatial resolution and so on. However, the temporal overlap of pump and Stokes has not been solved owing to the ultrafast optical pulse used in CARS microscopy. We combine interference spectrum of residual pump in Stokes path and nonlinear Schrodinger equation (NLSE) to realize the temporal overlap of pump pulse and Stokes pulse. At first, based on the interference spectrum of pump pulse and residual pump in Stokes path, the optical delay is defined when optical path difference between pump path and Stokes path is zero. Then the relative optical delay between Stokes pulse and residual pump in PCF can be calculated by NLSE. According to the spectrum interference and NLSE, temporal overlap of pump pulse and Stokes pulse will be realized easily and the imaging speed will be improved in CARS microscopy.
international conference on optical communications and networks | 2016
Tao Kuiyuan; Liu Tiegen; Ding Zhenyang; Zhou Yonghan; Liu Kun; Jiang Junfeng; Hu Haofeng; Kuang Hao; Liu Zixu
We present a Frequency-domain optical coherence tomography (FD-OCT) system for intravascular imaging. The whole system consists of 4 parts: imaging catheter (IC), motion controller (MC), optical engine (OE) and data acquisition and processing module (DAPM). By using swept laser source with 50 KHz sweep speed and high speed optical rotary jiont, we can get 100 frames per second (fps) and scan 20 mm vessel per second.
International Photonics and OptoElectronics Meetings (2014), paper JF2A.9 | 2014
Liu Wenhui; Tiegen Liu; Jiang Junfeng; Zhang Xuezhi; Yu Zhe; Chen Wenjie; Lin Xujun
Coupling from tapered fibers into the whispering gallery modes of the optofluidic ring resonator is investigated analytically. By adjusting the taper diameter to match the propagation constant of the mode in the taper with that of the resonant mode of interest, the mode with the best sensing capability can be excited selectively and efficiently.
Archive | 2014
Liu Tiegen; Liu Kun; Jiang Junfeng; Ding Zhenyang; Chen Qinnan; Sun Wei; Zhang Xiaoping; Li Dingjie
Archive | 2013
Jiang Junfeng; Liu Tiegen; Song Luyao; Liu Kun; Wang Shuang; Yin Jinde; He Pan
Archive | 2013
Jiang Junfeng; Liu Tiegen; Yin Jinde; Liu Kun; Wang Shuang; Wu Fan; Qin Zunqi; Song Luyao
Archive | 2015
Jiang Junfeng; Liu Tiegen; Yin Jinde; Liu Kun; Wang Shuang; Zou Shengliang; Qin Zunqi; Wu Fan
Archive | 2014
Jiang Junfeng; Liu Tiegen; Wang Shaohua; Liu Kun; Yin Jinde; Meng Xiange
Archive | 2013
Liu Kun; Liu Tiegen; Yu Lin; Jiang Junfeng; Song Luyao; Meng Yunxia; Wang Tao; Wang Ranran; Wang Liheng