Xin Yu

Xin Yu


Research Focus & Metrics

Academic Career Length

13Years (2014-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 October 2014 in Optics Express
Verified
Journal Article
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Yufei MaYufei Ma
Yufei Ma
XLXudong Li
Xudong Li
XYXin Yu
Xin Yu
RFRongwei Fan
Rongwei Fan
RYRenpeng Yan
Renpeng Yan
DCDeying Chen
Deying Chen
A novel miniaturized Cr4+:YAG passively Q-switched Nd:YAG pulse-burst laser under 808 nm diode-laser pulse-pumping was demonstrated for the purpose of laser-induced plasma ignition, in which pulse-burst mode can realize both high repetition rate and high pulse energy simultaneously in a short period. Side-pumping configuration and two different types of laser cavities were employed. The pumping pulse width was constant at 250 μs. For the plane-plane cavity, the output beam profile was flat-top Gaussian and the measured M2 value was 4.1 at the maximum incident pump energy of 600 mJ. The pulse-burst laser contained a maximum of 8 pulses, 7 pulses and 6 pulses for pulse-burst repetition rate of 10 Hz, 50 Hz and 100 Hz, respectively. The energy obtained was 15.5 mJ, 14.9 mJ and 13.9 mJ per pulse for pulse-burst repetition rate of 10 Hz, 50 Hz and 100 Hz, respectively. The maximum repetition rate of laser pulses in pulse-burst was 34.6 kHz for 8 pulses at the incident pump energy of 600 mJ and the single pulse width was 13.3 ns. The thermal lensing effect of Nd:YAG rod was investigated, and an plane-convex cavity was adopted to compensate the thermal lensing effect of Nd:YAG rod and improve the mode matching. For the plane-convex cavity, the output beam profile was quasi-Gaussian and the measured M2 value was 2.2 at the incident pump energy of 600 mJ. The output energy was 10.6 mJ per pulse for pulse-burst repetition rate of 100 Hz. The maximum repetition rate of laser pulses in pulse-burst was 27.4 kHz for 6 pulses at the incident pump energy of 600 mJ and the single pulse width was 14.2 ns. The experimental results showed that this pulse-burst laser can produce high repetition rate (>20 kHz) and high pulse energy (>10 mJ) simultaneously in a short period for both two different cavities.

22 April 2015 in Journal of Optics
Verified
Journal Article
Closed access
Yufei MaYufei Ma
Yufei Ma
GYGuang Yu
Guang Yu
JZJingbo Zhang
Jingbo Zhang
XYXin Yu
Xin Yu
RSRui Sun
Rui Sun

1 November 2015 in Chinese Physics B
Verified
Journal Article
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XYXin Yu
Xin Yu
ZYZhen Yang
Zhen Yang
JPJiang-Bo Peng
Jiang-Bo Peng
LZLei Zhang
Lei Zhang
YMYu-Fei Ma
Yu-Fei Ma
RSRui Sun
Rui Sun

9 August 2018 in Spectroscopy Letters
Verified
Journal Article
Closed access
GCGuang Chang
Guang Chang
JPJiangbo Peng
Jiangbo Peng
XYXin Yu
Xin Yu
HDHao Dong
Hao Dong
FDFan Deng
Fan Deng
XLXudong Li
Xudong Li
The research discussed the application of planar laser-induced fluorescence technique for visualizing the flow over an airfoil at different Reynolds numbers and angles of attack. The proposed arrangement allows visualizing the development process of the flow field structure around the airfoil. The focus of the study is the influence of the angles of attack and the Reynolds number on the separation boundary layer, which causes the wake vortex or separation bubble. Compared with the traditional visualization technology, the technology of planar laser-induced fluorescence has better time resolution (50 ns) and followability (Reynolds number = 219,500). In order to achieve high-speed flow field visualization, planar laser-induced fluorescence provides a reliable means of measurement to solve the related engineering problems.