利用平面双层远端荧光粉结构增强白光Led光通量

Doan Quoc Anh Nguyen, P. X. Le, Hsiao-Yi Lee
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引用次数: 4

摘要

本文比较了两种不同的双远端荧光粉结构——平面双远端荧光粉和凹形双远端荧光粉的光通量。结果表明,FDRP结构比CDRP结构更有利可图。在CDRP结构中,两个荧光粉层之间的距离(d1)和荧光粉层与LED表面之间的距离(d2)对光学性能有很大的影响。此外,d1和d2的差异导致远端荧光粉层的散射和吸收特性发生巨大变化,从而极大地影响了wled的照明能力和色彩均匀性。为了限制这些问题,wled的相关色温,本质上是衡量当“黑体”散热器加热到预定温度时观察到的色度,当d1和d2变化时,应该在8500K下平衡,需要适当修改YAG:Ce3+荧光粉的浓度。当d1 = d2 = 0时,远端荧光粉层的散射和同化变得最低,导致遮阳质量和虹彩过渡的生存能力下降最多,这取决于这两种分离不相同时产生的非地球影响。然后,当d1和d2变大时,色散面也变大,蓝色光束和黄色光束的混合振荡变得越来越均匀。这使得白光的差别不大,但不能达到光通量的增强。根据研究结果,光通量达到峰值1020 lm当d1或d2 = = 0.08毫米0.63毫米而色不均匀性达到最低点时d1或d2 = = 0.64毫米1.35 mm.This是一个开放存取物品分布条件下的知识共享归属许可(http://creativecommons.org/licenses/by/4.0/),它允许无限制的使用,在任何介质分布和繁殖提供了最初的工作是正确的引用。
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Enhanced Luminous Flux of White Led using Flat Dual-layer Remote Phosphor Configuration
The luminous flux of two different dual-remote phosphor structures concluding flat dual-remote phosphor (FDRP) and concave dual-remote phosphor (CDRP) is compared in this paper. The outcomes demonstrate that the FDRP structure is more lucrative than the CDRP structure. The article additionally clears up that in CDRP structure, the distance between two phosphor layers (d1) and the distance between the phosphor layer with the LED surface (d2) enormously affect the optical properties. Moreover, the difference in d1 and d2 causes a dramatic variance in the scattering and absorption properties of the remote phosphor layer and hence hugely affects WLEDs' illumination ability and chromatic uniformity. In order to limit these problems, the correlated color temperature of WLEDs, which is essentially a gauge of how the chromaticity observed when a "black body" radiator is warmed to a foreordained temperature, should be balanced out at 8500K when d1 and d2 vary, requiring a suitable modification of the YAG:Ce3+ phosphor's concentration. When d1 = d2 = 0, the scattering and assimilation in the remote phosphor layer become lowermost, prompting the most reduced viability in both shading quality and iridescent transition, which is confirmed dependent on the unearthly impacts created when these two separations are not same. Then again, when d1 and d2 get bigger, so does the dispersing surface, and the mixing of the blue beams with yellow beams swings to be increasingly homogeneous. This gives the insignificant different white light yet can't achieve any enhancement for luminous flux. According to the researched results, the luminous flux reaches a peak at 1020 lm when d1 = 0.08 mm or d2 = 0.63 mm whereas the chromatic inhomogeneity hits the lowest point when d1 = 0.64 mm or d2 = 1.35 mm.This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium provided the original work is properly cited.
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