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Comparison of nonpolar III-nitride vertical-cavity surface-emitting lasers with tunnel junction and ITO intracavity contacts

机译:具有隧道结和ITO腔内接触的非极性III氮化物垂直腔面发射激光器的比较

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摘要

We report on the lasing of III-nitride nonpolar, violet, vertical-cavity surface-emitting lasers (VCSELs) with III-nitride tunnel-junction (TJ) intracavity contacts and ion implanted apertures (IIAs). The TJ VCSELs are compared to similar VCSELs with tin-doped indium oxide (ITO) intracavity contacts. Prior to analyzing device results, we consider the relative advantages of III-nitride TJs for blue and green emitting VCSELs. The TJs are shown to be most advantageous for violet and UV VCSELs, operating near or above the absorption edge for ITO, as they significantly reduce the total internal loss in the cavity. However, for longer wavelength III-nitride VCSELs, TJs primarily offer the advantage of improved cavity design flexibility, allowing one to make the p-side thicker using a thick n-type III-nitride TJ intracavity contact. This offers improved lateral current spreading and lower loss, compare to using ITO and p-GaN, respectively. These aspects are particularly important for achieving high-power CW VCSELs, making TJs the ideal intracavity contact for any III-nitride VCSEL. A brief overview of III-nitride TJ growth methods is also given, highlighting the molecular-beam epitaxy (MBE) technique used here. Following this overview, we compare 12 mu m aperture diameter, violet emitting, TJ and ITO VCSEL experimental results, which demonstrate the significant improvement in differential efficiency and peak power resulting from the reduced loss in the TJ design. Specifically, the TJ VCSEL shows a peak power of similar to 550 mu W with a threshold current density of similar to 3.5 kA/cm(2), while the ITO VCSELs show peak powers of similar to 80 mu W and threshold current densities of similar to 7 kA/cm
机译:我们报道了具有III型氮化物隧道结(TJ)腔内接触和离子注入孔(IIA)的III型氮化物非极性,紫色,垂直腔表面发射激光器(VCSEL)的发射。将TJ VCSEL与具有掺杂锡的氧化铟(ITO)腔内触点的类似VCSEL进行了比较。在分析器件结果之前,我们考虑了III型氮化物TJ对于发射蓝色和绿色VCSEL的相对优势。示出的TJ对紫光和VCSEL最有利,它们在ITO的吸收边缘附近或上方工作,因为它们显着降低了腔体内的总内部损耗。但是,对于较长波长的III族氮化物VCSEL,TJ主要具有改进型腔设计灵活性的优势,允许使用厚的n型III型氮化物TJ腔内接触使p侧更厚。与分别使用ITO和p-GaN相比,这提供了改善的横向电流扩展和更低的损耗。这些方面对于实现大功率CW VCSEL尤其重要,这使TJ成为任何III型氮化物VCSEL的理想腔内接触。还简要介绍了III型氮化物TJ生长方法,重点介绍了此处使用的分子束外延(MBE)技术。在此概述之后,我们比较了孔径为12μm,紫光发射,TJ和ITO VCSEL的实验结果,这些结果表明,由于TJ设计损耗的减少,差分效率和峰值功率得到了显着改善。具体来说,TJ VCSEL的峰值功率类似于550μW,阈值电流密度类似于3.5 kA / cm(2),而ITO VCSEL的峰值功率类似于80μW,阈值电流密度近似至7 kA / cm

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