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Wafer bonding for optoelectronic devices.

机译:光电器件的晶圆键合。

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A periodic GaAs wafer-bonded structure has been proposed for quasi-phase-matched (QPM) second harmonic generation (SHG). The basic bonding technology involves elevated temperatures and pressures, which can lead to unacceptable optical losses and poor device performance. Three sources of optical losses were first found in this study: (1) decomposition at the exposed surface, (2) interfacial defects between the bonded wafers, and (3) bulk defects within the wafers.; Bulk and surface defects were studied by measuring the optical transmission through single GaAs. It was found that an increase in bonding temperature and/or time led to an increase in the bulk and surface defects. An increase in the free hole concentration (thermal conversion) is though to be the major cause of the optical losses by a free carrier absorption mechanism. Since it was difficult to eliminate free-carrier and interfacial defect losses once they have formed because of diffusion kinetic limitations, processing conditions that minimized their formation were sought. In contrast, defects on the external surfaces caused by arsenic depletion resulting from incongruent evaporation were easily eliminated by repolishing.; Interfacial defects were studied by introducing artificial voids into the interface region by bonding topographically-patterned GaAs wafers to unpatterned wafers. We found that the filling of these artificial voids depended strongly on the magnitude of the height of the surface irregularities on the wafer interfaces, as well as on temperature and time. Typically, when bonding temperature and time were increased, the interfacial defect density decreased. After bonding, two kinds of features corresponding to the newly bonded areas were observed by IR microscopy. These two features, having diamond and dendrite geometries, were shown to depend on both surface energy anisotropy and growth rate anisotropy.; An investigation of the relationship between bonding conditions (temperature, time and pressure) and optical losses (resulting from bulk, interfacial and surface defects), has led to the development of an optimized process for preparing periodic GaAs structures useful in quasi-phase-matched second harmonic generation applications. With this bonding process, low optical loss ({dollar}sim{dollar}0.1-0.3%/interface) wafer-bonded (110) structures (containing up to 40 layers) for practical device applications were first fabricated in this study.
机译:已经提出了一种周期性的砷化镓晶圆键合结构,用于准相位匹配(QPM)二次谐波产生(SHG)。基本的粘合技术涉及升高的温度和压力,这可能导致不可接受的光学损失和较差的器件性能。在这项研究中,首先发现了三种光学损耗源:(1)在裸露的表面上分解,(2)粘合晶片之间的界面缺陷,以及(3)晶片内部的整体缺陷。通过测量通过单个GaAs的光传输来研究体缺陷和表面缺陷。已经发现,键合温度和/或时间的增加导致体积和表面缺陷的增加。自由空穴浓度的增加(热转化)尽管是通过自由载流子吸收机制引起的光学损失的主要原因。由于由于扩散动力学的限制,一旦形成自由载流子和界面缺陷,就很难消除它们的损失,因此寻求将其形成最小化的加工条件。相反,由于不适当的蒸发而导致的砷耗竭引起的外表面缺陷可以通过重新抛光而消除。通过将构图图形化的GaAs晶片粘结到未构图的晶片上,通过在界面区域引入人工空隙来研究界面缺陷。我们发现,这些人造空隙的填充在很大程度上取决于晶片界面上表面不规则高度的大小,以及温度和时间。通常,当增加粘合温度和时间时,界面缺陷密度降低。结合后,通过红外显微镜观察到对应于新结合区域的两种特征。具有金刚石和枝晶几何形状的这两个特征显示出既取决于表面能各向异性又取决于生长速率各向异性。对键合条件(温度,时间和压力)与光学损耗(由于体积,界面和表面缺陷所致)之间的关系的研究,导致开发了一种用于制备可用于准相匹配的周期性GaAs结构的优化工艺。二次谐波的应用。通过这种键合工艺,本研究首先制造了用于实际器件应用的低光损耗({sim} {dollar} 0.1-0.3%/界面)的晶圆键合(110)结构(最多包含40层)。

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