β-Ga2O3(-201)衬底制备InGaN led

K. Iizuka, Y. Morishima, A. Kuramata, Yu-Jiun Shen, C. Tsai, Ying-Yong Su, Gavin Liu, T. Hsu, J. Yeh
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引用次数: 6

摘要

我们在β-Ga2O3(201)单晶衬底上制备了InGaN led。底物的生产采用边缘限定膜供生长(EFG)法。采用金属有机化学气相沉积(MOCVD)技术在导电β-Ga2O3(201)衬底上生长出掺硅GaN外延层。掺硅GaN层的x射线摇摆曲线(xrc)(0002)和(101)的半最大值全宽(FWHM)分别为220 arcsec和223 arcsec。阴极发光(CL)测量的暗斑密度约为1.5×108 cm-2。晶体质量与蓝宝石上的氮化镓层相当。我们制作了一个p面朝下的垂直LED。峰值波长约为450 nm。p接触金属面积为300 ×300 μm2。光输出功率在1000 A/cm2时未达到饱和。这一器件特性表明了Ga2O3在大功率led中应用的巨大潜力。
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InGaN LEDs prepared on β-Ga2O3 (-201) substrates
We fabricated InGaN LEDs prepared on β-Ga2O3 (201) single-crystal substrates. The substrates were produced by using the edge-defined film-fed growth (EFG) method. A Si-doped GaN epitaxial layer was grown on an electrically conductive β-Ga2O3 (201) substrate by metal organic chemical vapor deposition (MOCVD). The full-width at half maximum (FWHM) of (0002) and (101 1) X-ray rocking curves (XRCs) of the Si-doped GaN layer were 220 arcsec and 223 arcsec, respectively. The dark spot density measured by cathode luminescence (CL) was approximately 1.5×108 cm-2. The crystalline quality was equal to that of GaN layer on sapphire. We fabricated a vertical LED in the p-side down configuration. The peak wavelength was approximately 450 nm. The p-contact metal area was 300 ×300 μm2. The light output power did not saturate at 1000 A/cm2. This device characteristic indicates the great potential of Ga2O3 for use in high-power LEDs.
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