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    • 3. 发明申请
    • PLASMA SOURCE AND SURFACE TREATMENT METHOD
    • 等离子体源和表面处理方法
    • WO2015199539A1
    • 2015-12-30
    • PCT/NL2015/050463
    • 2015-06-25
    • NEDERLANDSE ORGANISATIE VOOR TOEGEPAST-NATUURWETENSCHAPPELIJK ONDERZOEK TNO
    • CREYGHTON, Yves Lodewijk MariaPOODT, Paulus Willibrordus GeorgeSIMOR, MarcelROOZEBOOM, Freddy
    • C23C16/455C23C16/513H01J37/32H05H1/24H01L21/314
    • C23C16/45514C23C16/45504C23C16/45536C23C16/4583C23C16/509C23C16/513H01J37/32348H01J37/32366H01J37/3244H01J37/32541H01J37/32568H01J37/32715H01J37/32825H01J2237/332H05H1/2406H05H2001/2412
    • Plasma source and surface treatment method. A plasma source has an outer surface (12), interrupted by an aperture (14) for delivering an atmospheric plasma from the outer surface. A transport mechanism (11) transports a substrate (10) in parallel with the outer surface, closely to the outer surface, so that gas from the atmospheric plasma may form a gas bearing between the outer surface the and the substrate. A first electrode (16a,b) of the plasma source has a first and second surface extending from an edge of the first electrode that runs along the aperture. The first surface defines the outer surface on a first side of the aperture. The distance between the first and second surface increasing with distance from the edge. A second electrode (17) covered at least partly by a dielectric layer (18) is provided with the dielectric layer facing the second surface of the first electrode, substantially in parallel with the second surface of the first electrode, leaving a plasma initiation space on said first side of the aperture, between the surface of the dielectric layer and the second surface of the first electrode. A gas inlet (19a,b) feeds into the plasma initiation space to provide gas flow from the gas inlet to the aperture through the plasma initiation space. Atmospheric plasma initiated in the plasma initiation space flows to the aperture, from which it leaves to react with the surface of the substrate.
    • 等离子体源和表面处理方法。 等离子体源具有由用于从外表面输送大气等离子体的孔(14)中断的外表面(12)。 输送机构(11)将与外表面平行的基板(10)紧密地输送到外表面,使得来自大气等离子体的气体可以在外表面和基板之间形成气体轴承。 等离子体源的第一电极(16a,b)具有从沿着孔径延伸的第一电极的边缘延伸的第一和第二表面。 第一表面限定孔的第一侧上的外表面。 第一和第二表面之间的距离随着与边缘的距离而增加。 至少部分地由电介质层(18)覆盖的第二电极(17)设置有介电层面向第一电极的第二表面,基本上与第一电极的第二表面平行,留下等离子体引发空间 所述孔的所述第一侧在介电层的表面和第一电极的第二表面之间。 气体入口(19a,b)进入等离子体引发空间,以通过等离子体引发空间提供从气体入口到孔的气流。 在等离子体起始空间中引发的大气等离子体流入孔,离开该孔与基板的表面反应。