基于两阶段光转换的叶片启发型发光太阳能聚光器的设计考虑

Hiroto Nishimura, K. Okada, Atsuya Suzuki, Yuta Mizuno, I. Fujieda
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引用次数: 0

摘要

光学聚光器的聚光系数定义为入射面和出射面光子通量的比值。它等于几何增益和光效率的乘积。放大发光太阳能聚光器(LSC)可以增加其几何增益,但由于聚光过程中光致发光(PL)光子的损失,其光学效率降低。在叶片LSC中,将发光光纤耦合到发光板的侧表面,使入射光子经过两段光转换。其几何增益急剧增加,但二次光转换过程降低了其光学效率。在实验中,在两块2mm厚的发光板之间放置一根直径为1.5 mm的纤维。光板发射绿色PL光子,光纤将它们转换成红色PL光子。利用直径为1 mm的激光在450nm波长处激发光斑,测量了光斑与位置相关的光效率。通过将板的横向尺寸从50 mm减小到10 mm,入射区域的平均光学效率从0.004增加到0.007。光线追踪模拟再现了测量结果。带弯弧耦合器的透明光波导可以将来自多个发光光纤的PL光子引导到光伏电池中。通过连接N个器件,预计几何增益将增加N倍,而光学效率保持不变。因此,这种配置为几何增益和光效率之间的权衡提供了一个解决方案。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Design considerations for leaf-inspired luminescent solar concentrators based on two-stage photoconversion
Concentration factor of an optical concentrator is defined as the ratio of photon fluxes at its incident and exiting surfaces. It is equal to the product of geometric gain and optical efficiency. Scaling up a luminescent solar concentrator (LSC) increases its geometric gain, but its optical efficiency decreases due to the loss of photoluminescence (PL) photons during the concentration process. In a leaf LSC, a luminescent fiber is coupled to the side surface of a luminescent plate such that an incident photon goes through two-stage photoconversion. Its geometric gain increases drastically but the second photoconversion process decreases its optical efficiency. In experiment, a 1.5 mm-diameter fiber was placed between two 2 mm-thick luminescent plates. The plates emitted green PL photons and the fiber converted them to red PL photons. Position-dependent optical efficiency was measured by exciting a single spot at various positions on the plate with a 1 mm-diameter laser light at 450 nm. The optical efficiency averaged over the incident area increased from 0.004 to 0.007 by decreasing the lateral size of the plate from 50 mm to 10 mm. Ray tracing simulations reproduced the measurement. A clear lightguide with arc-bend couplers can guide the PL photons from multiple luminescent fibers to a photovoltaic cell. By connecting N devices, N-fold increase in geometric gain is expected while the optical efficiency remains the same. Hence, this configuration provides a solution to the trade-off between geometric gain and optical efficiency.
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