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硅基板和铜基板垂直结构GaN基LED变温变电流发光性能的研究
引用本文:黄斌斌,熊传兵,张超宇,黄基锋,王光绪,汤英文,全知觉,徐龙权,张萌,王立,方文卿,刘军林,江风益. 硅基板和铜基板垂直结构GaN基LED变温变电流发光性能的研究[J]. 物理学报, 2014, 63(21): 217806-217806. DOI: 10.7498/aps.63.217806
作者姓名:黄斌斌  熊传兵  张超宇  黄基锋  王光绪  汤英文  全知觉  徐龙权  张萌  王立  方文卿  刘军林  江风益
作者单位:南昌大学国家硅基LED工程技术研究中心, 南昌 330047
基金项目:国家自然科学基金(批准号:51072076,11364034,61334001);国家高技术研究发展计划(批准号:2011AA03A101,2012AA041002);国家科技支撑计划(批准号:2011BAE32B01)资助的课题~~
摘    要:本文将硅(Si)衬底上外延生长的氮化镓(GaN)基发光二极管(LED)薄膜剥离转移到新的硅基板和紫铜基板上,并获得了垂直结构的LED芯片,对其变温变电流电致发光(EL)特性进行了研究. 结果表明:当环境温度不变时,在13 K低温状态下铜基板芯片的EL波长始终大于硅基板芯片约6 nm,在300 K 状态下随着驱动电流的加大铜基板芯片的EL波长会由大于硅基板芯片3 nm左右而逐渐变为与硅基板芯片重合;当驱动电流不变时,环境温度由13 K升高到320 K,两种基板芯片的EL波长随温度升高呈现S形变化并且波谱逐渐趋于重合;在100 K以下温度时铜基板芯片的Droop效应比硅基板芯片明显,在100 K 以上温度时硅基板芯片的Droop效应比铜基板芯片明显. 可能是由于两种芯片的基板具有不同的热膨胀系数和热导率导致了其变温变电流的EL特性不同.关键词:GaN热膨胀系数内量子效率热导率

关 键 词:GaN  热膨胀系数  内量子效率  热导率
收稿时间:2014-07-07

Electroluminescence properties of vertical structure GaN based LED on silicon and copper submount at different temperatures and current densities
Huang Bin-Bin,Xiong Chuan-Bing,Zhang Chao-Yu,Huang Ji-Feng,Wang Guang-Xu,Tang Ying-Wen,Quan Zhi-Jue,Xu Long-Quan,Zhang Meng,Wang Li,Fang Wen-Qing,Liu Jun-Lin,Jiang Feng-Yi. Electroluminescence properties of vertical structure GaN based LED on silicon and copper submount at different temperatures and current densities[J]. Acta Physica Sinica, 2014, 63(21): 217806-217806. DOI: 10.7498/aps.63.217806
Authors:Huang Bin-Bin  Xiong Chuan-Bing  Zhang Chao-Yu  Huang Ji-Feng  Wang Guang-Xu  Tang Ying-Wen  Quan Zhi-Jue  Xu Long-Quan  Zhang Meng  Wang Li  Fang Wen-Qing  Liu Jun-Lin  Jiang Feng-Yi
Abstract:GaN-based light-emitting diode (LED) thin films grown on Si(111) substrates are successfully detached and transferred to copper and silicon submounts, and then become 40mil high power vertical structure LED chips. Electroluminescence properties of the two kinds of chips with the same expitaxial structure are investigated at different forward current densities and ambient temperatures. The obtained results are as follows. 1) at the same temperature, the EL peak wavelength of the chip with copper submount is longer than that of the chip with silicon submount. Under 13 K, the EL peak wavelength of the chip with copper submount is about 6 nm longer than that of chip with silicon submount as the driving current increases from 0.01 mA to 400 mA. While under 300 K, the difference in EL peak wavelength between the two kinds of chips at 0.01 mA is only about 3 nm; as the current increases to 400 mA, the difference will tend to zero and the spectra will coincide. 2) At the same current density, as the temperature increases from 13 K to 320 K, the EL peak wavelengths of the two kinds of chips are S-shaped, and the spectra tend to coincide. 3)When the temperature is below 100 K, the current density droop effect of the chips with copper submount is more abvious than that of chips with silicon submount, while above 100 K, the results are just inverse. Perhaps, it is due to the fact that the differences in thermal expansion coefficient and thermal conductivity between the two kinds of submounts lead to the diffrent EL properties.
Keywords:GaNthermal expansion coefficientinternal quantum efficiencythermal conductivity
Keywords:GaN  thermal expansion coefficient  internal quantum efficiency  thermal conductivity
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