Two-dimensional condensation for uniaxially strained semiconductor fins
    162.
    发明授权
    Two-dimensional condensation for uniaxially strained semiconductor fins 有权
    用于单轴应变半导体翅片的二维冷凝

    公开(公告)号:US09159835B2

    公开(公告)日:2015-10-13

    申请号:US13488238

    申请日:2012-06-04

    Abstract: Techniques are disclosed for enabling multi-sided condensation of semiconductor fins. The techniques can be employed, for instance, in fabricating fin-based transistors. In one example case, a strain layer is provided on a bulk substrate. The strain layer is associated with a critical thickness that is dependent on a component of the strain layer, and the strain layer has a thickness lower than or equal to the critical thickness. A fin is formed in the substrate and strain layer, such that the fin includes a substrate portion and a strain layer portion. The fin is oxidized to condense the strain layer portion of the fin, so that a concentration of the component in the strain layer changes from a pre-condensation concentration to a higher post-condensation concentration, thereby causing the critical thickness to be exceeded.

    Abstract translation: 公开了用于实现半导体翅片的多面冷凝的技术。 这些技术可以用于例如制造基于鳍的晶体管。 在一个示例的情况下,在体基板上设置应变层。 应变层与取决于应变层的部件的临界厚度相关联,并且应变层具有低于或等于临界厚度的厚度。 在基板和应变层中形成翅片,使得翅片包括基板部分和应变层部分。 将翅片氧化以冷凝翅片的应变层部分,使得应变层中的组分的浓度从预凝结浓度变为较高的缩合后浓度,从而超过临界厚度。

    Strain-inducing semiconductor regions
    167.
    发明授权
    Strain-inducing semiconductor regions 有权
    应变诱导半导体区域

    公开(公告)号:US08841180B2

    公开(公告)日:2014-09-23

    申请号:US13971716

    申请日:2013-08-20

    Abstract: A method to form a strain-inducing semiconductor region is described. In one embodiment, formation of a strain-inducing semiconductor region laterally adjacent to a crystalline substrate results in a uniaxial strain imparted to the crystalline substrate, providing a strained crystalline substrate. In another embodiment, a semiconductor region with a crystalline lattice of one or more species of charge-neutral lattice-forming atoms imparts a strain to a crystalline substrate, wherein the lattice constant of the semiconductor region is different from that of the crystalline substrate, and wherein all species of charge-neutral lattice-forming atoms of the semiconductor region are contained in the crystalline substrate.

    Abstract translation: 描述形成应变诱导半导体区域的方法。 在一个实施方案中,形成横向邻近晶体衬底的应变诱导半导体区域导致赋予晶体衬底的单轴应变,从而提供应变的晶体衬底。 在另一个实施方案中,具有一种或多种电荷 - 中性晶格形成原子的晶格的半导体区域向晶体衬底赋予应变,其中半导体区域的晶格常数与晶体衬底的晶格常数不同,以及 其中所述半导体区域的电荷 - 中性晶格形成原子的所有种类都包含在所述晶体衬底中。

    NON-PLANAR GATE ALL-AROUND DEVICE AND METHOD OF FABRICATION THEREOF
    169.
    发明申请
    NON-PLANAR GATE ALL-AROUND DEVICE AND METHOD OF FABRICATION THEREOF 有权
    非平面门全部装置及其制造方法

    公开(公告)号:US20140225065A1

    公开(公告)日:2014-08-14

    申请号:US13997118

    申请日:2011-12-23

    Abstract: A non-planar gate all-around device and method of fabrication thereby are described. In one embodiment, the device includes a substrate having a top surface with a first lattice constant. Embedded epi source and drain regions are formed on the top surface of the substrate. The embedded epi source and drain regions have a second lattice constant that is different from the first lattice constant. Channel nanowires having a third lattice are formed between and are coupled to the embedded epi source and drain regions. In an embodiment, the second lattice constant and the third lattice constant are different from the first lattice constant. The channel nanowires include a bottom-most channel nanowire and a bottom gate isolation is formed on the top surface of the substrate under the bottom-most channel nanowire. A gate dielectric layer is formed on and all-around each channel nanowire. A gate electrode is formed on the gate dielectric layer and surrounding each channel nanowire.

    Abstract translation: 描述了非平面栅极全面器件及其制造方法。 在一个实施例中,该器件包括具有第一晶格常数的顶表面的衬底。 嵌入的epi源极和漏极区域形成在衬底的顶表面上。 嵌入的epi源极和漏极区具有不同于第一晶格常数的第二晶格常数。 具有第三晶格的沟道纳米线形成在嵌入的epi源极和漏极区之间并耦合到嵌入的epi源极和漏极区。 在一个实施例中,第二晶格常数和第三晶格常数不同于第一晶格常数。 通道纳米线包括最底部的沟道纳米线,并且在最底部的沟道纳米线下方的衬底的顶表面上形成底栅隔离。 在每个通道纳米线上形成栅极电介质层。 在栅极电介质层上形成栅电极并围绕每个沟道纳米线。

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