Polarization-engineered N-face III–V nitride quantum well LEDs

J. Verma, J. Simon, V. Protasenko, G. Xing, D. Jena
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Abstract

III–V nitride semiconductors are direct band gap semiconductors spanning a wide range of band gaps from 0.7 eV (InN, IR), through 3.4 eV (GaN, UV) to 6.2 eV (AlN, deep UV). This makes them uniquely suited for fabricating visible and UV LEDs [1]. UV LEDs have applications in water purification, microscopy and chemical analysis. However, wide band gap nitrides suffer from poor p-type doping owing to large activation energy of Mg acceptor dopant ( EA∼200 meV for GaN [2] and 650 meV for AlN [3]). This results in low thermal activation of holes at room temperature and causes low p-type conductivity. III–V nitrides also exhibit large built-in polarization field with spontaneous and strain induced piezoelectric components [4]. The polarization has recently been exploited to demonstrate N-face AlGaN/GaN p-n heterojunctions with improved p-type conductivities and electroluminescence [5]. In this work, we demonstrate that incorporating quantum wells (QWs) into the active regions improves electroluminescence (EL). Simultaneously, a number of advantages of N-face structures emerge from the point of view of polarization-engineering.
偏振工程n-面III-V氮化物量子阱led
III-V型氮化物半导体是直接带隙半导体,其带隙范围从0.7 eV (InN, IR)到3.4 eV (GaN, UV)到6.2 eV (AlN,深UV)。这使得它们非常适合制造可见光和紫外led[1]。UV led在水净化,显微镜和化学分析方面有应用。然而,由于Mg受体掺杂的活化能较大(GaN[2]为EA ~ 200 meV, AlN[3]为650 meV),宽带隙氮化物的p型掺杂效果较差。这导致孔在室温下的低热活化,并导致低p型电导率。III-V型氮化物也表现出较大的内置极化场,具有自发和应变诱导的压电元件[4]。最近,该极化被用来证明n面AlGaN/GaN p-n异质结具有改进的p型电导率和电致发光[5]。在这项工作中,我们证明了将量子阱(QWs)纳入有源区域可以改善电致发光(EL)。同时,从偏振工程的角度来看,n面结构具有许多优点。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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