Volume 47 Issue 12
Jan.  2019
Turn off MathJax
Article Contents
Article Navigation >  Infrared and Laser Engineering  > 2018  >  47(12): 1206005-1206005(5)

Luo Hao, Zhong Biao, Lei Yongqing, Shi Yanling, Yin Jianping. Thermal load management of laser cooling of Yb3+:LuLiF4 crystal[J]. Infrared and Laser Engineering, 2018, 47(12): 1206005-1206005(5). doi: 10.3788/IRLA201847.1206005
Citation: Luo Hao, Zhong Biao, Lei Yongqing, Shi Yanling, Yin Jianping. Thermal load management of laser cooling of Yb3+:LuLiF4 crystal[J]. Infrared and Laser Engineering, 2018, 47(12): 1206005-1206005(5). doi: 10.3788/IRLA201847.1206005
shu

Thermal load management of laser cooling of Yb3+:LuLiF4 crystal

doi: 10.3788/IRLA201847.1206005
  • 1.

    State Key Laboratory of Precision Spectroscopy,East China Normal University,Shanghai 200062,China;

  • 2.

    School of Information Science Technology,East China Normal University,Shanghai 200062,China

  • Received Date: 2018-07-11
  • Rev Recd Date: 2018-08-15
  • Publish Date: 2018-12-25
  • In order to study the thermal load management mechanism of Yb3+:LuLiF4 crystal in anti-Stokes fluorescence process, laser cooling experiment based on standard pressure (1.0105 Pa) and high vacuum(2.510-3 Pa) states were carried out. The 5 mol% doped sample was supported by two optical fibers, and was placed in chamber with different vacuum states. The sample was excited via a 1 020 nm, 3 W laser. A temperature drop from room temperature of the sample was about △T12 K under standard pressure, and △T26 K under high vacuum. As for standard pressure state, thermal convection load of air was about 11.23 mW, thermal conduction load of the fibers was about 0.03 mW, thermal radiation load of the chamber was about 4.8 mW. As for high vacuum state, convection load of air was about 0.03 mW, conduction load of the fibers was about 0.07 mW, radiation load of the chamber was about 10.4 mW. As experimental results show, with the decrease of the pressure of the chamber from -105 Pa to -103 Pa, convection load of air is almost negligible, radiation load of the chamber becomes the most important thermal load of the refrigeration sample.
  • [1] Pringsheim P. Zwei bemerkungen ber den Unterschied von Lumineszenz-und Temperaturstrahlung[J]. Z Phys, 1929, 57:739-746.
    [2] Seletskiy D V, Epstein R, Sheik-Bahae M, et al. Laser cooling in solids:advances and prospects[J]. Rep Prog Phys, 2016, 79(9):096401-096423.
    [3] Epstein R I, Buchwald M I. Observation of laser-induced fluorescence cooling of a solids[J]. Nature, 1995, 377:500-502.
    [4] Seletskiy D V, Sheik-Bahae M. Laser cooling of solids to cryogenic temperatures[J]. Nat Photonics, 2010, 4(3):161-164.
    [5] Zhang J, Xiong Q H. Laser cooling of semiconductor by 40 Kelvin[J]. Nature, 2013, 493:504-508.
    [6] Qin W P, Zhang J H. Two basic mechanism in anti-Stokes fluorescence cooling of solids[J]. Chinese Journal of Luminescence, 1999, 20(2):126-129. (in Chinese)
    [7] Dong G, Zhang X L. Energy transfer enhanced laser cooling in Ho3+ and Tm3+ co-doped lithium yttrium fluoride[J]. J Opt Soc Am B, 2013, 30(4):939-944.
    [8] Zhang J, Xiong Q H. Laser cooling of organic-inorganic lead halide perovskites[J]. Nat Photonics, 2016, 10(2):115-122.
    [9] Zhong B, Yin J P. Laser cooling of Yb3+-doped LuLiF4 crystal[J]. Opt Lett, 2014, 39(9):2747-2750.
    [10] Zhong B, Yin J P. Cavity-enhanced laser cooling for Yb3+-doped fluoride crystal using a low-power diode laser[J]. J Opt Soc Am B, 2014, 31(9):2116-2120.
    [11] Zhang C Q, Xu L. Study on anti-Stokes fluorescent cooling technique[J]. Infrared and Laser Engineering, 2002, 31(2):95-100. (in Chinese)
    [12] Fang H, Wu Yunong. Expectation of anti-Stokes fluorescence cooling to space remote sensing[J]. Chinese Journal of Quantum Electronics, 2004, 21(4):411-414. (in Chinese)
    [13] MHehlenP, Sheik-Bahae M, Epstein R I, et al. Materials for optical cryocoolers[J]. J Mater Chem C, 2013, 1:7471-7478.
    [14] Dong G Z. Research on novel mechanism for laser cooling of rare-earth doped fluoride crystals[D]. Harbin:Harbin Engineering University, 2015. (in Chinese)
    [15] Melgaard S D, Sheik-Bahae M. Solid state optical refrigeration to sub-100 Kelvin regime[J]. Sci Rep, 2016, 6:20380-20386.
    [16] Zhong B, Yin J P. Laser cooling of 5 mol% Yb3+:LuLiF4 crystal in air[J]. Opt Eng, 2017, 56(1):011102-011113.
    [17] Zhong B, Yin J P. Laser cooling performance of Yb3+-doped LuLiF4 crystal[C]//Proc SPIE, 2016, 9765:976506.
    [18] Jia Y H, Ji X M, Yin J P. Research on several parameters influencing on laser cooling of solids[J]. Acta Phys Sin, 2007, 56(3):1770-1774. (in Chinese)
    [19] Zhong B. Laser cooling of the Yb3+-doped fluoride crystal[D]. Shanghai:East China Normal University, 2014. (in Chinese)
    [20] Melgaard S D. Cryogenic optical refrigeration:laser cooling of solids below 123 K[D]. Albuquerque:University of New Mexico, 2013.
    [21] Yan X P, Wang D S. Summary of anti-Stokes fluorescent cooling technique[J]. Infrared and Laser Engineering, 2008, 37(3):474-480. (in Chinese)
    [22] Sheik-Bahae M, Epstein R I. Laser cooling of solids[J]. Laser Photonics Rev, 2009, 3(1-2):67-84.
    [23] Edwards B C, Epstein R I. Demonstration of a solid-state optical cooler:an approach to cryogenic refrigeration[J]. J Appl Phys, 1999, 86(11):6489-6493.
    [24] Imangholi B, Sheik-Bahae M, Epstein R I, et al. Differential luminescence thermometry in semiconductor laser cooling[C]//Proc SPIE, 2006, 6115:61151C.
  • 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
Get Citation
PDF
XML

Article Metrics

Article views(466) PDF downloads(33) Cited by()

Related
Proportional views

Thermal load management of laser cooling of Yb3+:LuLiF4 crystal

doi: 10.3788/IRLA201847.1206005
  • 1. State Key Laboratory of Precision Spectroscopy,East China Normal University,Shanghai 200062,China;
  • 2. School of Information Science Technology,East China Normal University,Shanghai 200062,China
  • Received Date: 2018-07-11
  • Rev Recd Date: 2018-08-15
  • Publish Date: 2018-12-25

Abstract: In order to study the thermal load management mechanism of Yb3+:LuLiF4 crystal in anti-Stokes fluorescence process, laser cooling experiment based on standard pressure (1.0105 Pa) and high vacuum(2.510-3 Pa) states were carried out. The 5 mol% doped sample was supported by two optical fibers, and was placed in chamber with different vacuum states. The sample was excited via a 1 020 nm, 3 W laser. A temperature drop from room temperature of the sample was about △T12 K under standard pressure, and △T26 K under high vacuum. As for standard pressure state, thermal convection load of air was about 11.23 mW, thermal conduction load of the fibers was about 0.03 mW, thermal radiation load of the chamber was about 4.8 mW. As for high vacuum state, convection load of air was about 0.03 mW, conduction load of the fibers was about 0.07 mW, radiation load of the chamber was about 10.4 mW. As experimental results show, with the decrease of the pressure of the chamber from -105 Pa to -103 Pa, convection load of air is almost negligible, radiation load of the chamber becomes the most important thermal load of the refrigeration sample.

    HTML

Reference (24)

Catalog

    版权所有 © 2019 《红外与激光工程》编辑部｜ Address: 58 Zhonghuan West Road, Tianjin Airport Economic Zone｜ Post Code: 300308

    津ICP备19007885号-1

    Supported by: Beijing Renhe Information Technology Co. Ltd  

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return