Xiaoyan Liang

Dr. Xiaoyan Liang


Research Focus & Metrics

Academic Career Length

16Years (2011-Present)

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

Representative Publications

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15 November 2018 in Optics Letters
Verified
Journal Article
Closed access
PDF file
WLWenqi Li
Wenqi Li
ZGZebiao Gan
Zebiao Gan
LYLianghong Yu
Lianghong Yu
CWCheng Wang
Cheng Wang
YLYanqi Liu
Yanqi Liu
ZXZhizhan Xu
Zhizhan Xu
We report on the laser pulse output of 339 J centered at 800 nm from a chirped-pulse amplification (CPA) Ti:sapphire laser system at the Shanghai Superintense Ultrafast Laser Facility. The experimental results demonstrated that the parasitic lasing as well as the transverse amplified spontaneous emission of the homemade 235-mm-diameter Ti:sapphire final amplifier were suppressed successfully via the temporal dual-pulse pumped scheme and the index-matching liquid cladding technique. The maximum pump-to-signal conversion efficiency of 32.1% was measured for the final amplifier. With a compressor transmission efficiency of 64% and a compressed pulse duration of 21 fs obtained for the sample light at a lower energy level, this laser system could potentially generate a compressed laser pulse with a peak power of 10.3 PW. The experimental results represent significant progress with respect to the CPA laser.

26 October 2015 in Optics Letters
Verified
Journal Article
Open access
PDF file
YCYuxi Chu
Yuxi Chu
ZGZebiao Gan
Zebiao Gan
XLXiaoyan Liang
Xiaoyan Liang
LYLianghong Yu
Lianghong Yu
XLXiaoming Lu
Xiaoming Lu
ZXZhizhan Xu
Zhizhan Xu
We report on the generation of 192.3 J centered at 800 nm wavelength from a chirped-pulse amplification (CPA) Ti:sapphire laser system. The experimental results demonstrate that parasitic lasing can be suppressed successfully in the final amplifier based on a Ti:sapphire crystal of 150 mm in diameter. An over 50% pump-to-signal conversion efficiency was measured for the final amplifier by optimizing the time delay of two pump pulses and enhancing the injected seed energy. With 72% compressor throughput efficiency and 27 fs long compressed pulse duration obtained at a lower energy level, this laser could potentially support a compressed laser pulse of 5.13 PW peak power. The experimental results represent notable progress regarding the CPA laser.

27 February 2017 in Optics Express
Verified
Journal Article
Open access
PDF file
ZGZebiao Gan
Zebiao Gan
LYLianghong Yu
Lianghong Yu
SLShuai Li
Shuai Li
CWCheng Wang
Cheng Wang
XLXiaoyan Liang
Xiaoyan Liang
ZXZhizhan Xu
Zhizhan Xu
We report on an experimental and theoretical study of a large-aperture Ti:Sapphire (Ti:S) amplifier pumped with a novel temporal dual-pulse scheme to suppress the parasitic lasing (PL) and transverse amplified spontaneous emission (TASE) for high-energy chirped-pulse amplification (CPA). The pump energy distribution was optimized and the time delay between each pump pulse was controlled precisely. Both the numerical and experimental results confirm that the temporal dual-pulse pump technique can effectively suppress PL and TASE. The maximum output energy of 202.8 J was obtained from the final 150-mm-diameter Ti:S booster amplifier with a pump energy of 320.0 J, corresponding to a conversion efficiency of 49.3%. The compressed pulse duration of 24.0 fs was measured with a throughput efficiency of 64%, leading to a peak power of 5.4 PW. This novel temporal dual-pulse pump technique has potential applications in a 10 PW CPA laser system.

28 September 2018 in Optics Express
Verified
Journal Article
Closed access
PDF file
ZGZhen Guo
Zhen Guo
LYLianghong Chen, Lianghong Yu
Lianghong Chen, Lianghong Yu
JWJianye Wang
Jianye Wang
CWCheng Wang
Cheng Wang
YLYanqi Liu
Yanqi Liu
RLRuxin Li
Ruxin Li
Double deformable mirrors (DMs) with different actuator densities are cascaded to optimize the wavefront aberrations to improve the focus intensity of the Shanghai super-intense ultrafast laser facility (SULF), which plans to generate 10 PW laser pulse. The beam aberrations near the focal spot are corrected from 0.556 um to 0.112 um in RMS by a 300-mm DM with a large stroke installed after the compressor. After then, it is further optimized to 0.041 um using a 130-mm DM with a high spatial resolution working after the main amplifier. The corrected beam is focused to 2.75 × 2.87 um2 at the full width at half maximum (FWHM) with an f/2.5 off-axis parabolic mirror (OAP), which contains approximately 27.69% energy. A peak intensity of 2 × 1022 W/cm2 is achieved at the output of 5.4 PW, and it could exceed 1023 W/cm2 in the SULF 10 PW laser facility using an f/1.8 OAP.

15 July 2015 in Optics Letters
Verified
Journal Article
Closed access
PDF file
LYLianghong Yu
Lianghong Yu
XLXiaoyan Liang
Xiaoyan Liang
LXLu Xu
Lu Xu
WLWenqi Li
Wenqi Li
CPChun Peng
Chun Peng
ZXZhizhan Xu
Zhizhan Xu
In this Letter, we present a study of high-energy and high-conversion-efficiency broadband optical parametric chirped-pulse amplification (OPCPA) system with a 100  mm×100  mm×17  mm LBO crystal near 800 nm. The results showed that the back-conversion was sensitively affected by the pump intensity and the injected signal intensity. It occurred when the injected signal was above 0.82 J with a pump energy of 170 J, and this effect also reshaped the amplified spectrum. After optimization, an amplified energy of 45.3 J was achieved with a conversion efficiency of 26.3% by the OPCPA. The peak power of the hybrid CPA-OPCPA laser system reached 1.02 PW with a compressed duration of 32 fs, which is the first reported OPCPA peak power higher than 1 PW, to the best of our knowledge.

26 July 2021 in Optics Letters
Verified
Journal Article
Closed access
PDF file
YZYuhang Zhang
Yuhang Zhang
SLShanming Li
Shanming Li
XDXiao Du
Xiao Du
JGJie Guo
Jie Guo
QGQiaorui Gong
Qiaorui Gong
YHYin Hang
Yin Hang
We present, to the best of our knowledge, the first demonstration of thermal, optical, and laser properties of Y b : G d S c O 3 for potentially efficient ultrashort pulse lasers. The stimulated emission cross section at 1025 nm (E//c) is 0.46 × 10 − 20 c m 2 with the emission band width of 85 nm, even broader than the well-known Y b : C a G d A l O 4 . It has quite a high thermal conductivity of 5.54 W / ( m ⋅ K ) at 50°C, comparable with Yb:YAG. In the continuous-wave regime, the maximum output power of 13.45 W at 1063.9 nm was generated with the optical-to-optical efficiency of 63.3%. These results suggest that the Y b : G d S c O 3 crystal is a promising candidate for ultrashort pulse lasers.