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Tensile Strained Ge Layers Obtained via a Si-CMOS Compatible Approach

机译:通过Si-CMOS兼容方法获得的拉伸应变GE层

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Although rapid advances in Si photonics over the last decade has enabled mass production of higher functionality and lower cost photonic components (such as waveguides, couplers, modulators, photodetectors, etc..) integrated with both digital and analog circuitry in silicon complementary metal oxide semiconductor technology (Si-CMOS), an efficient electrically-pumped light emitter integrated in the Si-CMOS has so far been considered the Holy Grail of the monolithic electronics-photonics integration. Among the different pathways leading to the on-chip integration of the light source, epitaxial lasers on silicon comprising active regions based on III-V or SiGe heterostructures have been proposed [1]. In particular Ge heteroepitaxial layers on Si are very promising since key photonic components for this material system, including high speed detectors and modulators, have already been successfully integrated in standard CMOS process flow. As a matter of fact, Ge is now a "fab"-compatible material deposited by means of fully qualified production processes and it is now considered one of the most promising material for "more than Moore" device development [2]. An optically pumped Ge-on-Si laser demonstrating CW operation at room temperature, has already been fabricated [3]. To achieve this goal, the authors exploited the small residual tensile strain (~0.2%) accumulated during the growth process and n-type doping. Although optical gain values as high as 1000 cm-1 are expected in such a system, the maximum gain reported so far is 50 cm-1, owing to the difficulties to achieve the n-doping density requested (~1020 cm-3) because donor solubility, dopant activation, and material processing issues. Increasing the tensile strain in to the Ge layer would allow to increase net optical gain value using easier-to-achieve donor density. Fabrication approaches based either on micromechanical engineering [4-7] or on the use of a str- ssor layer [8] have been successfully proposed. However, none of these methods are viable for a "true" monolithic integration in a CMOS foundry owing to either materials [6,8] or micro-fabrication and processing issues [4,5,7]. Here we present a fabrication method allowing to achieve high values of tensile strain in Ge layer deposited on a SOI substrate to be used as active material in light emitting devices. The fabrication process of the investigated structures has been carried out on 8" wafer using standard qualified CMOS-lithography process. A Ge layer deposited on a SOI substrate by means of production-grade CVD reactor is covered by highly compressively strained SiN layer acting as a stressor. Upon appropriate lithography of the SiN/Ge/SOI stack, micro-stripe and suspended micro-bridges such the one displayed in Fig. 1 are obtained. The relaxation of the compressive strain stored in to the SIN layer induces a tensile strain in to the Ge active layer. Micro-structures having sizes in the 10 to 1000 μm2 range and different orientation have been investigated in order to investigate the strain relaxation process as a function of geometry. Finite element method simulation and micro-Raman spectroscopy have been used to measure the strain distribution in to the micro-structure: values as high as ~1 % have been obtained. Room temperature photoluminescence (PL) is observed from these structures, giving evidence for strong direct-band related emission at wavelengths corresponding to those expected for the PL emission from tensile strained Ge layers. Figure 2 shows an example of PL spectrum of a microstripe structure as shown in Figure 1 (a). The luminescence is red-shifted as compared to the blanket structure because of tensile strain. Fabry-Perot oscillations due to reflections along t
机译:尽管在过去十年中的SI光子学的快速进展使得能够在硅互补金属氧化物半导体中集成的诸如数字和模拟电路的较高功能和低成本的光子元件(如波导,耦合器,调制器,光电探测器等)技术(SI-CMOS),在SI-CMOS中集成的有效电泵的光发射器已经被认为是整体电子 - 光子集成的圣杯。在导致光源的片上积分的不同途径中,已经提出了基于III-V或SiGe异质结构的有源区的硅上的外延激光[1]。特别是Si上的Ge异质轴层非常有希望,因为该材料系统的关键光子元件包括高速探测器和调制器,已经成功地集成在标准CMOS工艺流程中。事实上,GE现在是A" fab" - 通过完全合格的生产流程沉积的代替材料,现在被认为是&#x0022最有希望的材料之一;超过moore&#x0022 ;设备开发[2]。光学泵浦的GE-ON-SI激光器在室温下展示CW操作,已经制造了[3]。为了实现这一目标,作者利用在生长过程中累积的小残余拉伸菌株(〜0.2%)和n型掺杂。尽管在这样的系统中预期高达1000cm-1的光学增益值,但到目前为止报告的最大增益是50cm-1,由于难以实现所要求的n掺杂密度(〜1020cm-3),因为供体溶解度,掺杂剂活化和材料处理问题。增加GE层的拉伸应变将允许使用更容易实现的供体密度来增加净光学增益值。成功提出了基于微机械工程[4-7]或使用STR-SSOR层[8]的制造方法。但是,这些方法都不是A&#x0022的可行性;真实"由于材料[6,8]或微制造和处理问题,在CMOS铸造中的单片集成[4,5,7]。在这里,我们提出了一种制造方法,允许在SOI基板上沉积在SOI基板上的Ge层中的高值在发光器件中用作活性材料。已经在8&#X0022进行了研究的调查结构的制造过程;使用标准合格的CMOS光刻工艺晶圆。借助于生产级CVD反应器沉积在SOI衬底上的GE层被用作应力源的高度压缩性紧张的SIN层覆盖。在SIN / GE / SOI堆叠的适当光刻,如图1所示的微条纹和悬浮微桥。存储在SiN层中的压缩菌株的松弛引起了GE活性层的拉伸应变。已经研究了在10至1000μm2范围内的尺寸和不同取向的微结构,以便作为几何形状的函数研究应变弛豫过程。有限元方法模拟和微拉曼光谱已经用于测量微结构的应变分布:高达〜1%的值。从这些结构观察到室温光致发光(PL),提供对应于与拉伸应变GE层的PL发射的预期的波长的强烈直接带相关发射的证据。图2示出了如图1(a)所示的微带结构的PL光谱的示例。由于拉伸应变,与橡皮布结构相比,发光是红移。由于T的反射,法布里 - 珀罗振荡

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