High-Efficiency Diode-Resonantly-Pumped Tm:Lu2O3 Ceramic Laser with Near Diffraction-Limited Beam Quality

Author(s):  
Wensheng Zhang ◽  
Linjun Li ◽  
Sheng Zhou ◽  
Qiong Gao
2022 ◽  
pp. 1-1
Author(s):  
Yu Liu ◽  
Shan Huang ◽  
Wenjie Wu ◽  
Lianghua Xie ◽  
Chun Zhang ◽  
...  

2021 ◽  
Vol 18 (8) ◽  
pp. 085004
Author(s):  
Chen Song ◽  
Yun Wang ◽  
Houwen Yang ◽  
Dazhen Li ◽  
Wenyong Cheng

2020 ◽  
Vol 8 ◽  
Author(s):  
Ning Ma ◽  
Meng Chen ◽  
Ce Yang ◽  
Shang Lu ◽  
Xie Zhang ◽  
...  

We report high-energy, high-efficiency second harmonic generation in a near-infrared all-solid-state burst-mode picosecond laser at a repetition rate of 1 kHz with four pulses per burst using a type-I noncritical phase-matching lithium triborate crystal. The pulses in each burst have the same time delay ( ${\sim}1~\text{ns}$ ), the same pulse duration ( ${\sim}100~\text{ps}$ ) and different relative amplitudes that can be adjusted separately. A mode-locked beam from a semiconductor saturable absorber mirror is pulse-stretched, split into seed pulses and injected into a Nd:YAG regenerative amplifier. After the beam is reshaped by aspheric lenses, a two-stage master oscillator power amplifier and 4f imaging systems are applied to obtain a high power of ${\sim}100~\text{W}$ . The 532 nm green laser has a maximum conversion efficiency of 68%, an average power of up to 50 W and a beam quality factor $M^{2}$ of 3.5.


2013 ◽  
Vol 35 (4) ◽  
pp. 804-806 ◽  
Author(s):  
Yuwan Zou ◽  
Zhiyi Wei ◽  
Qing Wang ◽  
Minjie Zhan ◽  
Dehua Li ◽  
...  

2012 ◽  
Vol 529 ◽  
pp. 105-109 ◽  
Author(s):  
X.F. Wang ◽  
Z.W. Fan ◽  
J. Yu ◽  
Z.H. Shi ◽  
T.Z. Zhao ◽  
...  

To obtain high energy, high efficiency Nd: glass preamplifier used in certain host device, a Nd:glass regenerative amplifier system has been designed. By adjusting the single pass gain and carefully optimizing the cavity mode, the small-scale self-focusing effect in the gain medium was effectively controlled. Maximum pulse energy of 21mJ, pulse width of 2.6ns was obtained at the repetition frequency of 1Hz, corresponding to a high optical to optical conversion efficiency of 11% and amplification ratio of 108. The pulse to pulse energy stability was < 2% rms during 2 h continous operation. The laser has a good beam quality of M2=1.5. The spectrum was measured to be at center wavelength of 1052.915nm.


2013 ◽  
Vol 321-324 ◽  
pp. 482-485
Author(s):  
Zhi Chao Wu ◽  
Xiu Li Zhang

The Nd:YAG ceramic laser at 670 nm was studied by means of dispersion prism and KTP intracavity-frequency-doubling. We designed and optimized the cavity parameters by MatrixLaser software based on the standard ABCD ray propagation matrix. By using the laser diode arrays side-pumped Nd:YAG ceramic crystal with Nd doping concentration of 1.1at% and dimension of Φ3×50 mm, the Nd:YAG ceramic laser at 670 nm was realized. Under repetition rate of 1 000Hz and single pulse pumped energy of 144 mJ, the output energy of 5.1mJ at 670 nm is obtained. The optic-optic efficiency is 3.54%. The results not only formed the basis for the further development of the high power and high efficiency ceramic red laser, but also provided a great prospect for the high power ceramic red laser in the field of medical treatment, color display and other areas of application.


2017 ◽  
Vol 56 (10) ◽  
pp. 2804 ◽  
Author(s):  
Kai Liu ◽  
Chun Zhao ◽  
Yifeng Yang ◽  
Xiaolong Chen ◽  
Jianhua Wang ◽  
...  

2021 ◽  
pp. 52-56
Author(s):  
V.I. Maslov ◽  
R.T. Ovsiannikov ◽  
D.S. Bondar ◽  
I.P. Levchuk ◽  
I.N. Onishchenko

Plasma wakefield acceleration promises compact sources of high-brightness relativistic electron and positron beams. Applications (particle colliders and free-electron lasers) of plasma wakefield accelerators demand low ener-gy spread beams and high-efficiency operation. Achieving both requires plateau formation on both the accelerating field for witness-bunch and the decelerating fields for driver-bunches by controlled beam loading of the plasma wave with careful tailored current profiles. We demonstrate by numerical simulation by 2.5D PIC code LCODE such optimal beam loading in a linear and blowout electron-driven plasma accelerator with RF generated low and high beam charge and high beam quality.


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