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    • 2. 发明申请
    • LPP EUV LIGHT SOURCE
    • LPP EUV光源
    • WO2005089131A2
    • 2005-09-29
    • PCT/US2005/007063
    • 2005-03-03
    • CYMER, INC.PARTLO, William, N.BROWN, Daniel, J., W.FOMENKOV, Igor, V.BOWERING, Norbert, R.RETTIG, Curtis, L.MACFARLANE, Joseph, J.ERSHOV, Alexander, I.HANSSON, Bjorn, A., M.
    • PARTLO, William, N.BROWN, Daniel, J., W.FOMENKOV, Igor, V.BOWERING, Norbert, R.RETTIG, Curtis, L.MACFARLANE, Joseph, J.ERSHOV, Alexander, I.HANSSON, Bjorn, A., M.
    • G03F7/20H05G2/00
    • H05G2/003B82Y10/00G03F7/70033H01S3/0085H01S3/0092H01S3/1611H01S3/1653H01S3/2255H01S3/2325H01S3/2375H01S3/2383H05G2/005H05G2/008
    • An apparatus and method is described for effectively and efficiently providing plasma irradiation laser light pulses in an LPP EUV light source which may comprise a laser initial target irradiation pulse generating mechanism irradiating a plasma initiation target with an initial target irradiation pulse to form an EUV generating plasma having an emission region emitting in-band EUV light; a laser plasma irradiation pulse generating mechanism irradiating the plasma with a plasma irradiation pulse after the initial target irradiation pulse so as to compress emission material in the plasma toward the emission region of the plasma. The plasma irradiation pulse may comprise a laser pulse having a wavelength that is sufficiently longer than a wavelength of the initial target irradiation .pulse to have an associated lower critical density resulting in absorption occurring within the plasma in a region of the plasma defined by the wavelength of the plasma irradiation pulse sufficiently separated from an initial target irradiation site to achieve compression of the emission material, and the may compress the emission region. The laser plasma irradiation pulse may produce an aerial mass density in the ablating cloud of the plasma sufficient to confine the favorably emitting plasma for increased conversion efficiency. The deposition region for the plasma irradiation pulse may be is removed enough from the initial target surface so as to insure compression of the favorably emitting plasma. A high conversion efficiency laser produced plasma extreme ultraviolet (“EUV”) light source may comprise a laser initial target irradiation pulse generating mechanism irradiating a plasma initiation target with a target irradiation pulse to form an EUV generating plasma emitting in-band EUV light; a plasma tamper substantially surrounding the plasma to constrain the expansion of the plasma.
    • 描述了一种用于在LPP EUV光源中有效且有效地提供等离子体照射激光脉冲的装置和方法,其可以包括用初始目标照射脉冲照射等离子体引发目标的激光初始靶照射脉冲发生机构以形成产生EUV的等离子体 具有发射带内EUV光的发射区域; 激光等离子体照射脉冲发生机构在初始目标照射脉冲之后用等离子体照射脉冲照射等离子体,以将等离子体中的发射材料压缩到等离子体的发射区域。 等离子体照射脉冲可以包括具有足够长于初始靶照射脉冲的波长的波长的激光脉冲,以具有相关联的较低临界密度,从而在由波长限定的等离子体区域内的等离子体内发生吸收 的等离子体照射脉冲与初始靶照射部位充分分离,以实现发射材料的压缩,并且可以压缩发射区域。 激光等离子体照射脉冲可以在等离子体的消融云中产生足够的空气质量密度以限制有利的发射等离子体以提高转换效率。 可以从初始目标表面去除等离子体照射脉冲的沉积区域,以确保有利地发射等离子体的压缩。 高转换效率的激光产生的等离子体极紫外(“EUV”)光源可以包括激光初始靶照射脉冲发生机构,用目标照射脉冲照射等离子体引发目标,以形成产生EUV的发射等离子体的带内EUV光; 等离子体篡改基本上围绕等离子体以约束等离子体的膨胀。
    • 10. 发明申请
    • COLLECTOR FOR EUV LIGHT SOURCE
    • EUV光源收集器
    • WO2004092693A2
    • 2004-10-28
    • PCT/US2004/010972
    • 2004-04-07
    • CYMER, INC.PARTLO, William, N.ALGOTS, J., MartinBLUMENSTOCK, Gerry, M.BOWERING, NorbertERSHOV, Alexander, I.FOMENKOV, Igor, V.PAN, Xiaojiang, J.
    • PARTLO, William, N.ALGOTS, J., MartinBLUMENSTOCK, Gerry, M.BOWERING, NorbertERSHOV, Alexander, I.FOMENKOV, Igor, V.PAN, Xiaojiang, J.
    • G01J
    • H05G2/001B82Y10/00G03F7/70033G03F7/70175G03F7/70916G21K1/062
    • A method and apparatus for debris removal from a reflecting surface of an EUV collector in an EUV light source is disclosed which may comprise the reflecting surface comprises a first material and the debris comprises a second material and/or compounds of the second material, the system and method may comprise a controlled sputtering ion source which may comprise a gas comprising the atoms of the sputtering ion material; and a stimulating mechanism exciting the atoms of the sputtering ion material into an ionized state, the ionized state being selected to have a distribution around a selected energy peak that has a high probability of sputtering the second material and a very low probability of sputtering the first material. The stimulating mechanism may comprise an RF or microwave induction mechanism. The gas is maintained at a pressure that in part determines the selected energy peak and the stimulating mechanism may create an influx of ions of the sputtering ion material that creates a sputter density of atoms of the second material from the reflector surface that equals or exceeds the influx rate of the plasma debris atoms of the second material. A sputtering rate may be selected for a given desired life of the reflecting surface. The reflecting surface may be capped. The collector may comprise an elliptical mirror and a debris shield which may comprise radially extending channels. The first material may be molybdenum, the second lithium and the ion material may be helium. The system may have a heater to evaporate the second material from the reflecting surface. The stimulating mechanism may be connected to the reflecting surface between ignition times. The reflecting surface may have barrier layers. The collector may be a spherical mirror in combination with grazing angle of incidence reflector shells, which may act as a spectral filter by selection of the layer material for multi-layer stacks on the reflector shells. The sputtering can be in combination with heating, the latter removing the lithium and the former removing compounds of lithium, and the sputtering may be by ions produced in the plasma rather than excited gas atoms.
    • 公开了一种用于从EUV光源中的EUV收集器的反射表面去除碎片的方法和装置,其可以包括反射表面,其包括第一材料,并且所述碎屑包括第二材料和/或第二材料的化合物,所述系统 并且方法可以包括受控的溅射离子源,其可以包括包含溅射离子材料的原子的气体; 以及将溅射离子材料的原子激发成离子化状态的刺激机构,所选择的离子化状态具有围绕选择的能量峰的分布,其具有溅射第二材料的可能性很高,并且溅射的可能性非常低 材料。 刺激机构可以包括RF或微波感应机构。 气体保持在部分地决定所选择的能量峰值的压力下,并且刺激机构可以产生溅射离子材料的离子的流入,其从反射器表面产生第二材料的原子的溅射密度等于或超过 第二种材料的等离子体碎片原子的流入速率。 可以在反射表面的给定期望寿命期间选择溅射速率。 反射面可以被盖住。 收集器可以包括椭圆镜和可包括径向延伸通道的碎片屏蔽。 第一材料可以是钼,第二锂和离子材料可以是氦。 该系统可以具有从反射表面蒸发第二材料的加热器。 刺激机构可以在点火时间之间连接到反射表面。 反射表面可以具有阻挡层。 收集器可以是与入射反射器壳的掠射角组合的球面镜,其可以通过选择反射器壳体上的多层堆叠的层材料来充当光谱滤光器。 溅射可以与加热相结合,后者除去锂和前者除去锂的化合物,并且溅射可以是在等离子体中产生的离子而不是被激发的气体原子。