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Compact, distributed inductive element for large scale inductively-coupled plasma sources

机译:紧凑的分布式电感元件,用于大规模电感耦合等离子体源

摘要

An inductively coupled plasma source is provided with a compact inductive element that is configured to produce a spatially distributed plasma particularly suitable for processing large scale wafers. The element in its preferred embodiment is formed of a sheet material for compactness and ease in configuring. The element is located outside of a dielectric wall or window of a processing chamber, generally congruent to the dielectric wall or window, formed of one or more layers or loops. The conductor provides a conductive path around each loop that has a serpentine or oscillating configuration that renders the path around each loop greater than the circumference of the element. The path is so shaped by cutouts along the side edges of the element. The conductor is formed of alternating sections of large and small aspect ratio, defined as the width across the path to the thickness of the sheet. The sections are also defined by cutouts in the sheet. Narrower sections concentrate currents, have higher inductances, and couple greater amounts of energy into the chamber, thereby producing rings of discrete plasma concentrations. One or more rings can be produced by configuring one or more loops of the inductive element so the higher inductance, lower aspect ratio sections lie at appropriate radii from the axis of the chamber.
机译:感应耦合等离子体源设有紧凑的感应元件,该紧凑的感应元件被配置为产生特别适合于处理大规模晶片的空间分布的等离子体。在其优选实施例中,该元件由片状材料形成,以紧凑且易于构造。该元件位于处理室的电介质壁或窗口的外部,通常与电介质壁或窗口同等,由一个或多个层或环形成。导体在每个回路周围提供一条具有蛇形或振荡配置的导电路径,从而使每个回路周围的路径大于元件的周长。这样的路径是通过沿元素的侧边缘的切口来成形的。导体由纵横比大和小的交替部分形成,长宽比定义为横跨路径的宽度到薄片的厚度。这些部分也由图纸中的切口定义。较窄的部分集中电流,具有较高的电感,并将更多的能量耦合到腔室内,从而产生离散的等离子体浓度的环。可以通过配置电感元件的一个或多个回路来产生一个或多个环,这样,较高的电感,较低的宽高比部分位于距腔室轴线适当的半径处。

著录项

  • 公开/公告号US2005160985A1

    专利类型

  • 公开/公告日2005-07-28

    原文格式PDF

  • 申请/专利权人 JOZEF BRCKA;

    申请/专利号US20040766505

  • 发明设计人 JOZEF BRCKA;

    申请日2004-01-28

  • 分类号C23C16/00;

  • 国家 US

  • 入库时间 2022-08-21 22:24:22

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