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    • 1. 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。