首页> 外文会议>International Silicon-Germanium Technology and Device Meeting >Strained High Percentage (60) Boron Doped Silicon-Germanium Alloys - Strain, Dopant Substitionality, Carrier Concentration, Resistivity, and Microstructure Development
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Strained High Percentage (60) Boron Doped Silicon-Germanium Alloys - Strain, Dopant Substitionality, Carrier Concentration, Resistivity, and Microstructure Development

机译:应变高百分比(60%)硼掺杂硅 - 锗合金 - 菌株,掺杂剂分子,载体浓度,电阻率和微观结构发育

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Future generations of silicon based integrated circuit technology require carrier concentrations in excess of the equilibrium dopant concentrations. Implantation is not the dopant method of choice anymore, since the structures get smaller and thinner with each technology node, additional three-dimensional structures being introduced with FinFET as one option for the 22 nm node [1]. Implantation into thin semiconductor structures will amorphize them and relax eventual strain in them. In-situ doping during the epitaxial growth is an alternate way to deposit dopants where you need them in concentrations desired and avoid the problems associated with implantation. In this work we study the incorporation of boron into fully strained high percentage (60%) boron doped Silicon-Germanium (SiGe). We will discuss the epitaxial growth, dopant incorporation, and strain compensation due to the dopant atoms, defect generation in highly strained doped SiGe layers as well as dopant activation, free carrier concentration and mobilities. We will look at band structure effects due to high doping in strained SiGe layers. The studied SiGe films were epitaxially deposited at low temperature to achieve high doping levels and avoid thermally induced relaxation. At those low deposition temperatures we observed high dopant incorporation with perfect crystal quality. A thickness range of 20 to 27 nm was chosen to retain a fully strained layer while allowing sufficient material for physical and electrical analyses. Doping levels reach from 3?1019cm-3 to 1.5?1021cm-3 and higher. At the higher doping levels three-dimensional growth is observed, which leads to pronounced relaxation (Figure 1). From highly n-doped silicon it is known, that not all substitutional incorporated phosphorus is electrically active, since it forms donor dimers [2]. These dimers electrically deactivate the phosphorus, but still contribute to the lattice contraction. We also observe a high lattice contraction- measured here as strain compensation, from the added boron atoms. The existence of similar boron acceptor dimers is imaginable, which would lead to less electrical active dopants than the total substitutional incorporated dopant. Hall measurements on boron doped 60% SiGe showed that the carrier density is significantly higher than the boron doping concentration determined by SIMS. Mobilities are very low with 30 cm2/V sec as example for the 1x1020 cm-3 boron doped sample. We will explain these effects and draw conclusions for the band structure and density of states in doped 60% SiGe. This work was performed by the Research Alliance Teams at various IBM Research and Development Facilities.
机译:未来几代基于硅的集成电路技术需要超过平衡掺杂剂浓度的载体浓度。植入不是掺杂剂的选择方法,因为该结构与每个技术节点变得较小和更薄,因此使用FinFET引入额外的三维结构作为22nm节点的一个选项[1]。植入到薄的半导体结构中将它们是混合它们并在它们中放松最终的应变。在外延生长期间的原位掺杂是沉积掺杂剂的交替方式,在其中需要以所需的浓度,避免与植入相关的问题。在这项工作中,我们研究了硼的结合到完全应变高百分比(60%)硼掺杂硅锗(SiGe)。我们将讨论由于掺杂剂原子引起的外延生长,掺杂剂掺入和应变补偿,高度应变的掺杂SiGe层以及掺杂剂活化,游离载体浓度和迁移率。由于紧张的SiGe层中的高掺杂,我们将看看带结构效应。将研究的SiGe膜在低温下外延沉积,以达到高掺杂水平并避免热诱导的松弛。在那些低沉积温度下,我们观察到具有完美晶体质量的高掺杂剂。选择20至27nm的厚度范围以保持完全应变层,同时允许足够的材料进行物理和电气分析。掺杂水平达到3. 1019cm-3至1.5?1021cm-3和更高。在较高的掺杂水平下,观察到三维生长,这导致松弛松弛(图1)。从高度N掺杂的硅中,已知,并非所有的掺入磷都是电活性的,因为它形成供体二聚体[2]。这些二聚体导致磷,但仍然有助于晶格收缩。我们还观察到这里测量的高晶格收缩作为应变补偿,从添加的硼原子中测量。类似的硼受体二聚体的存在是可想而想的,这将导致电活性掺杂剂较少,而不是总取代掺入掺杂剂。硼的霍尔测量掺杂60%SiGE显示,载体密度显着高于SIMS测定的硼掺杂浓度。迁移率非常低,用30cm2 / v秒为例,例如1×1020 cm-3硼掺杂样品的示例。我们将解释这些效果并得出掺杂60%SiGe中的状态的频带结构和密度的结论。这项工作由研究联盟团队在各种IBM研究和开发设施进行。

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