Dongzhen Li

Dr. Dongzhen Li

orcid

Research Focus & Metrics

Academic Career Length

17Years (2010-Present)

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

Representative Publications

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9 October 2019 in Optical Materials Express
Verified
Journal Article
Closed access
PDF file
DWDongHai Wang
DongHai Wang
WHWenTao Hou
WenTao Hou
NLNa Li
Na Li
YXYanYan Xue
YanYan Xue
QWQingGuo Wang
QingGuo Wang
JXJun Xu
Jun Xu
Cr-doped GdScO3 single crystals were grown by the EFG method. Based on their absorption and emission spectras, the crystal field strength and the crystal field parameters of the octahedrally-coordinated Cr3+ ions were determined: Dq = 1553 cm-1, B = 574 cm-1, C = 3211 cm-1, and Dq/B = 2.71 for 0.5% Cr:GdScO3. Effective phonon energy was calculated to be 412 cm−1, and the Huang–Rhys factor was 3.0. The emission spectra of Cr3+ doped GdScO3 crystal covered the region from 650 nm to 1100 nm, and the emission cross-section at 767 nm was calculated to be 0.32×10−20 cm2. In comparison with the other Cr3+ doped materials, the Cr:GdScO3 crystal has a short fluorescence lifetime, it can be used as a potential tunable laser gain medium.

22 March 2018 in Materials
Verified
Journal Article
Open access
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JLJun Liu
Jun Liu
PLPeng Liu
Peng Liu
JWJun Wang
Jun Wang
XXXiaodong Xu
Xiaodong Xu
DLDongzhen Li
Dongzhen Li
XNXinming Nie
Xinming Nie
In this paper, we report the fabrication of high-quality 5 at. % Er3+ ions doped SrF2 transparent ceramics, the potential candidate materials for a mid-infrared laser-gain medium by hot-pressing at 700 °C for 40 h using a chemically-derived powder. The phase structure, densification, and microstructure evolution of the Er:SrF2 ceramics were systematically investigated. In addition, the grain growth kinetic mechanism of Er:SrF2 was clarified. The results showed lattice diffusion to be the grain growth mechanism in the Er:SrF2 transparent ceramic of which highest in-line transmittance reached 92% at 2000 nm, i.e., very close to the theoretical transmittance value of SrF2 single crystal. Furthermore, the emission spectra showed that the strongest emission band was located at 2735 nm. This means that it is possible to achieve a laser output of approximately 2.7 μm in the 5 at. % Er3+ ions doped SrF2 transparent ceramics.

12 August 2019 in Optics Express
Verified
Journal Article
Closed access
DLDongzhen Li
Dongzhen Li
LKLingchen Kong
Lingchen Kong
XXXiaodong Xu
Xiaodong Xu
PLPeng Liu
Peng Liu
GXGuoqiang Xie
Guoqiang Xie
JXJun Xu
Jun Xu
Tm:LuYO3 mixed ceramic was successfully fabricated by the solid-state reactive sintering method. The absorption cross section and emission cross section were studied at room temperature. The fluorescence lifetime of 3F4 energy level was fitted to be 2.6 ms. A continuous-wave (CW) laser operation of Tm:LuYO3 ceramic, pumped at 796 nm, was realized with the output power of 1.2 W and slope efficiency of 25.1%. A mode-locking (ML) laser operation of Tm:LuYO3 ceramic was demonstrated for the first time with pulse duration of 41 ps and pulse repetition frequency of 139.3 MHz.

8 February 2022 in Optics Express
Verified
Journal Article
Closed access
JLJian Liu
Jian Liu
QSQingsong Song
Qingsong Song
ZWZhanxin Wang
Zhanxin Wang
YWYinyin Wang
Yinyin Wang
JDJifei Dong
Jifei Dong
Yongguang zhaoYongguang zhao
Yongguang zhao
Lutetium aluminum garnet single-crystal fiber (SCF, ∼ Φ 0.9 mm – 165 mm) doped with 0.5 at.% Ho3+ has been grown by the micro-pulling-down (µ-PD) technique. The room-temperature absorption and emission spectra exhibit similar features to the bulk crystal. Laser performances of the SCFs with two different pump configurations, i.e., pump guiding and free-space propagation, are studied by employing a 1.9-µm laser diode and a high-brightness fiber laser, respectively. Laser slope efficiencies obtained with both pump configurations can be higher than 50%, and a maximum output power of 6.01 W is achieved at ∼ 2.09 µm with the former pump. The comparable efficiency to the high-brightness pump is an indication of that high laser performance can also be expected through pump-guiding in the SCF even with a low pump beam quality.

11 January 2022 in Optical Materials Express
Verified
Journal Article
Closed access
WWWudi Wang
Wudi Wang
JTJie Tian
Jie Tian
NLNa Li
Na Li
JLJian Liu
Jian Liu
DHDonghua Hu
Donghua Hu
JXJun Xu
Jun Xu
Pr3+-doped GdScO3 single crystal was successfully grown by the Czochralski (Cz) method. Polarized absorption spectra, polarized fluorescence spectra, and fluorescence decay curves were measured at room temperature. The polarized spectroscopic property of Pr:GdScO3 crystal for new-wavelength transition in the near infrared (NIR) region was discussed for the first time. The absorption cross-sections at 600 nm were calculated to be 0.39×10−20 cm2 (E∥a), 0.32×10−20 cm2 (E∥b) and 0.4×10−20 cm2 (E∥c). The emission cross sections at 1053 nm of 1D2 energy level were calculated to be 0.86×10−20 cm2 (E∥a), 0.79×10−20 cm2 (E∥b) and 0.78×10−20 cm2 (E∥c), with FWHM of 57.54 nm, 57.96 nm and 58.96 nm, respectively. The fluorescence lifetime and radiative lifetime of the 1D2 energy levels of Pr3+ ions were 45.46 µs and 393.94 µs, respectively. Those results show that the Pr:GdScO3 crystal should be the potential near infrared laser gain medium originated from the 1D2 transition.

9 November 2018 in Applied Optics
Verified
Journal Article
Closed access
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YPYuxin Pan
Yuxin Pan
SZShidong Zhou
Shidong Zhou
JWJiawei Wang
Jiawei Wang
BXBin Xu
Bin Xu
JLJian Liu
Jian Liu
JXJun Xu
Jun Xu
A Nd3+-doped LaMgAl11O19 (Nd:LMA) crystal was grown by the Czochralski method. Room temperature polarized absorption spectra, fluorescence spectra, and fluorescence lifetime of the Nd:LMA crystal were measured and analyzed. The Judd–Ofelt parameters Ω2,4,6 were calculated to be 1.21×10−20, 3.63×10−20, and 2.35×10−20  cm2, respectively. The absorption and emission cross sections were calculated. Using a 790-nm diode laser as pump source, continuous-wave laser operation of an a-cut Nd:LMA crystal has been demonstrated with a maximum output power of 1.71 W and slope efficiency of 40.4% for a 1055 nm laser. Low-gain laser operation at 1082 nm is also realized with a maximum output power of 1.46 W and slope efficiency of 34.5%.