Gain performance and thermal effects of Nd:Glass and Nd,Y:SrF<sub>2</sub> crystal

The gain performance and thermal effects of Nd:glass (N31) and Nd,Y:SrF 2 crystal are investigated and compared. The results show that, under the same pump conditions, Nd,Y:SrF 2 can provide a small-signal gain similar to that of N31. The main advantages of Nd,Y:SrF 2 are its weaker thermal effects and greater thermal-fracture limitations compared with those of N31. In this paper, the two gain media are compared in the form of rods whose diameter is 5 mm and length is 60 mm. The small-signal gain coefficients of N31 and Nd,Y:SrF 2 are 1.39 and 1.46, respectively, at a pump energy of 1.5 J/1 Hz. The pump energy is set at 1.5 J/8 Hz to experimentally investigate their thermal effects. The thermal wavefront of N31 is 0.987λ at a repetition rate of 10 Hz, whereas that of Nd,Y:SrF 2 is 0.679 λ . In thermal destructive experiments, N31 fractured at an average pump power of 15 W (1.5 J/10 Hz), whereas Nd,Y:SrF 2 fractured at a higher power of 27 W (1.5 J/18 Hz) owing to its excellent thermal conductivity, which is 7.28 times that of N31. These results indicate the potential of Nd,Y:SrF 2 crystal as a gain medium for high-repetition-rate laser amplifiers.

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Publication Details

Journal
Applied Optics
Published
2024-09-16
DOI
https://doi.org/10.1364/ao.539514
Citations
1
Primary Topic
Metallurgical Processes and Thermodynamics
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article
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article

Gain performance and thermal effects of Nd:Glass and Nd,Y:SrF2 crystal

Dapeng Jiang, Zhen Zhang, Liangbi Su, Xinghua Lu et al.
1 citations
Applied Optics
Metallurgical Processes and Thermodynamics
0.21
article

Gain performance and thermal effects of Nd:Glass and Nd,Y:SrF2 crystal

Dapeng Jiang, Zhen Zhang, Liangbi Su, Xinghua Lu, Jiangtao Guo, Wei Fan, Jiangfeng Wang, Xuechun Li, Xiaochao Wang, Yenan Zhang
article en
1 citations

Abstract

The gain performance and thermal effects of Nd:glass (N31) and Nd,Y:SrF 2 crystal are investigated and compared. The results show that, under the same pump conditions, Nd,Y:SrF 2 can provide a small-signal gain similar to that of N31. The main advantages of Nd,Y:SrF 2 are its weaker thermal effects and greater thermal-fracture limitations compared with those of N31. In this paper, the two gain media are compared in the form of rods whose diameter is 5 mm and length is 60 mm. The small-signal gain coefficients of N31 and Nd,Y:SrF 2 are 1.39 and 1.46, respectively, at a pump energy of 1.5 J/1 Hz. The pump energy is set at 1.5 J/8 Hz to experimentally investigate their thermal effects. The thermal wavefront of N31 is 0.987λ at a repetition rate of 10 Hz, whereas that of Nd,Y:SrF 2 is 0.679 λ . In thermal destructive experiments, N31 fractured at an average pump power of 15 W (1.5 J/10 Hz), whereas Nd,Y:SrF 2 fractured at a higher power of 27 W (1.5 J/18 Hz) owing to its excellent thermal conductivity, which is 7.28 times that of N31. These results indicate the potential of Nd,Y:SrF 2 crystal as a gain medium for high-repetition-rate laser amplifiers.

Applied OpticsVol. 63(30)
Chinese Academy of Sciences (CN), Shanghai Institute of Optics and Fine Mechanics (CN), Shanghai Institute of Ceramics (CN), University of Chinese Academy of Sciences (CN)
Affordable and clean energy
Openalex Percentile: Top 52%
Metallurgical Processes and Thermodynamics
0.21
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