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Microcavity light emitting diodes in the visible red and near infrared wavelength range

机译:可见红色和近红外波长范围内的微腔发光二极管

摘要

It was about 125 years ago that the light bulb was commercialized by Thomas Edison. No doubt a brilliant invention at the time, today its low power conversion efficiency is one of the reasons why lighting in the western world has such high energy consumption. Thus, the potential for saving energy is enormous in this area. The introduction of halogen, discharge and fluorescent lamps has lead to certain efficiency improvements, however more than half of the energy is still lost as heat. Light-emitting diodes (LEDs) are very promising candidates for high efficiency light sources, with modern devices showing internal quantum efficiencies of virtually 100 %. However, due to the high refractive index of the commonly used semiconductor materials it is very difficult to have a large extraction efficiency; in a standard cubic geometry most of the internally emitted light is trapped inside the device due to total internal reflection. Several methods have been developed in order to circumvent this problem, either by optimizing the device geometry in order to increase the escape cone or by incorporating a resonant structure in order to force the internal emission into the existing escape cone. The latter approach is called microcavity LED (MCLED) or resonant cavity LED (RCLED). In a MCLED the spontaneous internal emission is controlled by placing the emitter inside an optical cavity with a thickness of the order of its emitting wavelength. The resulting interference effects increase the part of the emission that can be extracted. Contrary to the other approaches this is possible without changing the device geometry and thus without additional costly back-end processing steps. The control of the farfield radiation pattern makes these devices particularly interesting for high brightness applications, which demand highly directional emitters, such as for printing, bar code reading, large area displays and optical communication. The extraction efficiency of a MCLED is inversely proportional to the effective cavity length. An ideal cavity, allowing an extraction efficiency close to unity, consists of a low refractive index material and has an optical length of λ/2. In contrast to this, to obtain high internal quantum efficiencies it is necessary to use high index cavities with an optical length of at least λ. It should be noted, that the large penetration depth of the optical field in the semiconductor-based distributed Bragg reflectors (DBRs) leads to a significant increase of the effective cavity length and thus further reduces the achievable extraction efficiencies. In this thesis novel concepts to reduce effective cavity lengths and therefore increase extraction efficiencies are implemented into standard MCLED structures. The phaseshift cavity principle whilst maintaining the electrical properties of a standard A cavity achieves optical properties approaching that of a λ/2 cavity. The use of AlOx instead of AlAs as the, low refractive index component in the DBRs leads to smaller penetration depths and a concomitant reduction of the effective cavity length. A similar effect can be obtained by combining a resonant cavity with a thin-film structure. Thanks to these design improvements, the external quantum efficiency of different types of MCLEDs was increased. Near infrared emitting InGaAs/GaAs MCLEDs including a phase-shift cavity were realized, as both bottom and top emitting structures. The external quantum efficiencies achieved for emission into air were 18 and 19 %, respectively. With the additional incorporation of an oxide based bottom DBR, the efficiency of top emitting near infrared MCLEDs was further increased to 28 %. Red emitting AlGaInP-based structures are not compatible with the phase-shift cavity principle. However the beneficial effect of the implementation of an oxide DBR is greater at their wavelength rather than in the near infrared. Thus with preliminary red emitting GaInP/AlGaInP MCLEDs containing a bottom oxide DBR external quantum efficiencies of 12% could be achieved. Unfortunately, the incorporation of an oxide DBR significantly complicates the device design and the device fabrication. These problems can be avoided by combining the resonant cavity with a thin-film structure instead. Initial non-optimized red emitting thin-film MCLEDs were realized by OSRAM Opto Semiconductors and characterized in this work. They show external quantum efficiencies of 23 % and 18 % with and without encapsulation, respectively. It is assumed that a significant fraction of the high external quantum efficiency is due to a strong photon recycling effect in these devices. Simulations presented in this thesis show that the theoretical limits for the MCLEDs discussed above are slightly higher than the values obtained, encouraging further device optimization. The thin-film MCLEDs seem to hold the biggest potential for high efficiency emission from MCLEDs, independent of the wavelength range of emission.
机译:大约125年前,托马斯·爱迪生(Thomas Edison)将灯泡商业化。毫无疑问,这是当时的一项杰出发明,如今,它的低功率转换效率是西方照明如此高能耗的原因之一。因此,在该领域节省能源的潜力是巨大的。卤素灯,放电灯和荧光灯的引入带来了一定的效率提高,但是仍有一半以上的能量作为热量损失掉了。发光二极管(LED)是高效光源的非常有希望的候选者,现代设备显示出的内部量子效率几乎为100%。然而,由于常用的半导体材料的高折射率,很难具有大的提取效率。在标准的立方几何形状中,大多数内部发射的光由于全内反射而被捕获在设备内部。为了解决这个问题,已经开发了几种方法,或者通过优化装置的几何形状以增加逃生锥,或者通过引入谐振结构以迫使内部发射进入现有的逃生锥中来解决该问题。后一种方法称为微腔LED(MCLED)或谐振腔LED(RCLED)。在MCLED中,通过将发射器放置在光学腔体中来控制自发内部发射,该光学腔体的厚度约为其发射波长。产生的干扰效应增加了可以提取的发射部分。与其他方法相反,这是可能的,而无需更改设备的几何形状,因此无需其他昂贵的后端处理步骤。远场辐射方向图的控制使这些设备特别适合高亮度应用,这些应用需要高度定向的发射器,例如用于打印,条形码读取,大面积显示和光通信。 MCLED的提取效率与有效腔体长度成反比。理想的腔体,其提取效率接近于1,由低折射率材料组成,并且光学长度为λ/ 2。与此相反,为了获得高的内部量子效率,必须使用光学长度至少为λ的高折射率腔。应该注意的是,在基于半导体的分布式布拉格反射器(DBR)中,光场的大穿透深度导致有效腔体长度的显着增加,从而进一步降低了可达到的提取效率。在本论文中,减少有效腔体长度并因此提高提取效率的新颖概念已在标准MCLED结构中实现。相移腔原理在保持标准A腔电学特性的同时,实现了接近λ/ 2腔的光学特性。在DBR中使用AlOx代替AlAs作为低折射率成分会导致更小的穿透深度,并同时减少有效腔体长度。通过将谐振腔与薄膜结构相结合可以获得类似的效果。由于这些设计改进,提高了不同类型的MCLED的外部量子效率。作为底部和顶部发射结构,实现了具有相移腔的近红外发射InGaAs / GaAs MCLED。排放到空气中的外部量子效率分别为18%和19%。通过额外加入氧化物基底部DBR,顶部发射近红外MCLED的效率进一步提高到28%。发射红光的基于AlGaInP的结构与相移腔原理不兼容。然而,实施氧化物DBR的有益效果在其波长处而不是在近红外处更大。因此,利用包含底部氧化物DBR的预先发射红色的GaInP / AlGaInP MCLED,可以实现外部量子效率为12%。不幸的是,氧化物DBR的掺入显着使器件设计和器件制造复杂化。这些问题可以通过将谐振腔与薄膜结构结合起来来避免。最初的未经优化的发红光薄膜MCLED由欧司朗光电半导体实现,并在这项工作中得到了表征。它们显示有和没有封装的外部量子效率分别为23%和18%。据推测,高外部量子效率的很大一部分是由于这些器件中强大的光子回收效应所致。本文提出的仿真结果表明,以上讨论的MCLED的理论极限值略高于获得的值,这鼓励了进一步的器件优化。薄膜MCLED似乎拥有从MCLED高效发射的最大潜力,而与发射的波长范围无关。

著录项

  • 作者

    Joray Reto;

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  • 年度 2005
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  • 原文格式 PDF
  • 正文语种 eng
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