Advanced Search

ISSN1001-3806 CN51-1125/TN Map

Volume 37 Issue 4
May  2013
Article Contents
Turn off MathJax

Citation:

Laser systems pumped by sunlight directly and computer simulation optimization

  • Corresponding author: ZHAO Chang-ming, zhaochangming@bit.edu.cn
  • Received Date: 2012-11-09
    Accepted Date: 2012-12-03
  • In order to achieve the conversion from the sunlight to the laser, two-level aggregation experimental system was designed and built. By choosing a Fresnel lens as the first level of aggregation system, the diffuse reflectance tapered cavity as the second level of aggregation system and Nd:YAG as the working substance, the experimental maximum power output was 13.3W available, when the sunlight incident power was about 950W/m2. In order to optimize the experimental system and improve the power output, the resonant cavity was simulated by LASCAD software. The temperature distribution and the refractive index distribution during the working of the crystal rod were obtained. The system was optimized by changing the parameters. The variation of the output power along with the cavity length and the output mirror reflectivity, the best cavity length of 142mm and the output mirror reflectivity of 91% were obtained. The results show that the output power of the laser pumped by sunlight directly can be improved effectively by adjusting the cavity length and the output mirror reflectivity and the best value can be achieved.
  • 加载中
  • [1]

    LUO P P,LIU Ch,XU P,et al. Solar pumped Nd:YAG laser with Fresnel Lens[J]. Chinese Journal of Lasers,2011,38(10):1002002(in Chinese).
    [2]

    SIMPSON G R.Continuous sun-pumped room temperature glass laser operation[J]. Applied Optics,1964,36(7): 1671-1678.
    [3]

    YOUNG C G. A sun-pumped CW one-watt laser[J]. Applied Optics,1966,5(6):993-998.
    [4]

    WEKSLER M, SHWARTZ J. Solar-pumped solid-state lasers[J]. IEEE Journal of Quantum Electronics,1988,QE24(6):1222-1228.
    [5]

    YABE T, BAGHERI B, OHKUBO T,et al. 100W-class solar pumped laser for sustainable magnesium-hydrogen energy cycle[J]. Journal of Applied Physics,2008,104(8):083104.
    [6]

    LIANG D W, ALMEIDA J. Highly efficient solar-pumped Nd:YAG laser[J]. Optics Express,2011,19(27):26399-26405.
    [7]

    DINH T H, OHKUBO T, YABE T,et al. 120watt continuous wave solar-pumped laser with a liquid light-guide lens and an Nd:YAG rod[J].Optics Letters,2012,37(13):2670-2672.
    [8]

    ZHANG Q,WANG Y F,HOU J Y,et al. Simulation and experimentation of high power high repetition U folded resonator laser[J].High Power Laser and Particle Beams,2011,23(4):943-948(in Chinese).
  • 加载中
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Article views(4115) PDF downloads(852) Cited by()

Proportional views

Laser systems pumped by sunlight directly and computer simulation optimization

    Corresponding author: ZHAO Chang-ming, zhaochangming@bit.edu.cn
  • 1. School of Optoelectronics, Beijing Institude of Technology, Beijing 100081, China

Abstract: In order to achieve the conversion from the sunlight to the laser, two-level aggregation experimental system was designed and built. By choosing a Fresnel lens as the first level of aggregation system, the diffuse reflectance tapered cavity as the second level of aggregation system and Nd:YAG as the working substance, the experimental maximum power output was 13.3W available, when the sunlight incident power was about 950W/m2. In order to optimize the experimental system and improve the power output, the resonant cavity was simulated by LASCAD software. The temperature distribution and the refractive index distribution during the working of the crystal rod were obtained. The system was optimized by changing the parameters. The variation of the output power along with the cavity length and the output mirror reflectivity, the best cavity length of 142mm and the output mirror reflectivity of 91% were obtained. The results show that the output power of the laser pumped by sunlight directly can be improved effectively by adjusting the cavity length and the output mirror reflectivity and the best value can be achieved.

Reference (8)

Catalog

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return