首页> 外文会议>Optical components and materials XIV >Thermal conductivity investigation of Adhesive-Free Bond laser components
【24h】

Thermal conductivity investigation of Adhesive-Free Bond laser components

机译:无胶粘结激光组件的导热系数研究

获取原文
获取原文并翻译 | 示例

摘要

An interferometric method has been developed and employed at Onyx Optics, Inc. to accurately measure the thermal conductivity of laser-active crystals as function of dopant concentration or inactive materials such as single crystals, optical ceramics and glasses relative to a standard of assumed to be known thermal conductivity [1]. This technique can also provide information on heat transfer resistance at the interface between two materials in close thermal contact. While the technique appears generally applicable to composites between optically homogeneous materials, we report on thermal conductivities and heat transfer coefficients of selected adhesive-free bond (AFB®) laser composites. Single crystal bars and AFB bonded crystal doublets with the combinations of various rare-earth (Nd~(3+), Yb~(3+), Er~(3+) and Tm~(3+)trivalent ion doped YAG, and un-doped YAG have been fabricated with the AFB technique. By loading the test sample in a vacuum cryostat, with a precisely controlled heat load at one end of the doublets, the temperature distribution inside the single crystal or the composite samples can been precisely mapped by measuring the optical path difference interferometrically, given the material's thermal-optical properties. No measurable heat transfer resistance can be identified for the AFB interfaces between low-concentration doped YAG and un-doped YAG. For the heavily doped RE~(3+):YAG, for example, 10% Yb:YAG, the thermal conductivity measured in our experiment is 8.3 W/m·K, using the thermal conductivity of undoped YAG reported in [1] as basis. The thermal transfer resistance of the AFB interface with un-doped YAG, if there is any at the AFB interface, could be less than 1.29×10~(-6) m~2·K/W.
机译:Onyx Optics,Inc.已开发并采用了一种干涉测量方法,以相对于假定的标准,精确地测量激光活性晶体的热导率,该热导率随掺杂剂浓度或非活性材料(如单晶,光学陶瓷和玻璃)的变化而变化。已知的热导率[1]。该技术还可以提供有关紧密接触的两种材料之间的界面处的传热阻力的信息。尽管该技术似乎普遍适用于光学均质材料之间的复合材料,但我们报告了选定的无粘合剂激光复合材料的热导率和传热系数。单晶棒和AFB键合晶体双峰结合了多种稀土元素(Nd〜(3 +),Yb〜(3 +),Er〜(3+)和Tm〜(3+)三价离子掺杂YAG和用AFB技术制造未掺杂的YAG,通过将测试样品加载到真空低温恒温器中,并在双峰的一端精确控制热负荷,可以精确地绘制单晶或复合样品内部的温度分布在给定材料的热光学特性的情况下,通过干涉测量光程差,无法确定可测量的低浓度YAG和未掺杂YAG之间的AFB界面的传热阻力;对于重掺杂RE〜(3+) :[YAG],例如10%Yb:YAG,我们在实验中测得的热导率为8.3 W / m·K,以[1]中报告的未掺杂YAG的热导率为基础。对于未掺杂的YAG,如果AFB接口处有任何掺杂,小于1.29×10〜(-6)m〜2·K / W。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号