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闽南师范大学 物理与信息工程学院,福建 漳州 363000
[ "李晓珍(1993-),女,广东揭西人,硕士研究生,2017年于牡丹江师范学院获得学士学位,主要从事半导体发光器件的研究。 E-mail: jxlixiaozhen@163.com" ]
[ "熊传兵(1973-),男,江西南昌人,博士,教授,2008年于南昌大学获得博士学位,主要从事LED和半导体激光器的研究。 E-mail:chuanbingxiong@126.com" ]
纸质出版日期:2021-09-01,
收稿日期:2021-05-27,
修回日期:2021-06-11,
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李晓珍, 熊传兵, 汤英文, 等. 大功率倒装LED芯片陶瓷封装器件顶面微区发光均匀性[J]. 发光学报, 2021,42(9):1436-1445.
Xiao-zhen LI, Chuan-bing XIONG, Ying-wen TANG, et al. Uniformity of Light Emission in Micro-area on Mesa of High-power Flip-chip LED Devices with Ceramic Packaging[J]. Chinese Journal of Luminescence, 2021,42(9):1436-1445.
李晓珍, 熊传兵, 汤英文, 等. 大功率倒装LED芯片陶瓷封装器件顶面微区发光均匀性[J]. 发光学报, 2021,42(9):1436-1445. DOI: 10.37188/CJL.20210199.
Xiao-zhen LI, Chuan-bing XIONG, Ying-wen TANG, et al. Uniformity of Light Emission in Micro-area on Mesa of High-power Flip-chip LED Devices with Ceramic Packaging[J]. Chinese Journal of Luminescence, 2021,42(9):1436-1445. DOI: 10.37188/CJL.20210199.
高功率密度的陶瓷封装LED器件在大电流工作时,其顶面发光均匀性是该类器件的关键指标。本文在3.5 mm×3.5 mm的氮化铝陶瓷基板上金锡共晶了1.905 mm×1.830 mm(75 mil×72 mil)的LED倒装蓝光大功率芯片,然后分别制作成蓝光器件和白光器件,并分别对器件顶面的微区发光均匀性进行了研究。结果表明,蓝光器件在电流<3 A时,其顶面光强分布均匀,均匀性受N电极孔和电极间隙的影响较小;在4~8 A电流时,蓝光器件顶面光强分布不均匀,贯穿N电极孔测试区的光强大于电极孔之间测试区的光强,电极间隙区光强最低,离N电极孔越远的测试点光强越低;蓝光器件在8 A时整体光强达到饱和,而不同微区的光饱和程度及峰值波长随电流的变化有所不同;白光器件在0~4 A电流时,其顶面光强分布均匀。
The uniformity of light emission on the top surface of high-power-density LED devices with ceramic packages is a key indicator of this type of device when working at high currents. In this paper
the blue high-power LED flip chip(1.905 mm×1.830 mm(75 mil×72 mil)) is soldered on an aluminum nitride ceramic substrate(3.5 mm×3.5 mm) through Au-Sn eutectic welding
and then were made into white light emitting device and blue light components. The uniformity of micro-area luminescence on the top surface of these devices was also studied. The results show that when the current is less than 4 A
the light intensity distribution on the top surface of the blue device is uniform
and the uniformity is less affected by the N electrode hole and the electrode gap. When the current is 4-8 A
the light intensity distribution on the top surface of the blue light device is uneven. The light passing through the test area of the N electrode hole is stronger than the light intensity of the test area between the electrode holes. The light intensity of the electrode gap area is the lowest
which is far from the N electrode hole. The farther the test point
the lower the light intensity. The overall light intensity of the blue light device reaches saturation at 8 A
but the degree of light saturation and peak wavelength of different micro-area vary with the current change; when the white light device is at a current of 0-4 A
the light intensity distribution on its top surface is uniform.
微区发光倒装芯片电极孔电极间隙
micro-luminescenceflip chipelectrode holeelectrode gap
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