会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 5. 发明申请
    • LASER OUTPUT BEAM WAVEFRONT SPLITTER FOR BANDWIDTH SPECTRUM CONTROL
    • 激光输出波束分波器用于带宽频谱控制
    • WO2006009905A1
    • 2006-01-26
    • PCT/US2005/021585
    • 2005-06-17
    • CYMER, INC.SANDSTROM, Richard, L.BROWN, Daniel, J., W.ERSHOV, Alexander, I.FOMENKOV, Igor, V.PARTLO, William, N.
    • SANDSTROM, Richard, L.BROWN, Daniel, J., W.ERSHOV, Alexander, I.FOMENKOV, Igor, V.PARTLO, William, N.
    • H01S3/22
    • H01S3/0812G03F7/70025G03F7/70575H01S3/08059H01S3/097H01S3/1055H01S3/1305
    • An apparatus and method for providing bandwidth control in a narrow band short pulse duration gas discharge laser output light pulse beam producing system, producing a beam comprising laser output light pulses at a selected pulse repetition rate, is disclosed which may comprise a dispersive bandwidth selection optic (Fig. 1, character 120) selecting at least one center wavelength for each pulse determined at least in part by the angle (of incidence of the laser light pulse beam containing the respective pulse on the dispersive wavelength selection optic; a tuning mechanism operative to select at least one angle ( Δα L)of incidence of the a laser light pulse beam containing the respective pulse upon the dispersive center wavelength selection optic; the tuning mechanism comprising a plurality of incidence angle selection elements each defining an angle of incidence for a different spatially separated but not temporally separated portion of the laser light pulse to return from the dispersive center wavelength selection optic a laser light pulse comprising a plurality of spatially separated but not temporally separated portions, each portion having one of at least two different selected center wavelengths. The tuning mechanism may comprise a temporal angle ( Δα L) of incidence selection element defining an angle of incidence for different temporally separated portions of the pulse to return from the dispersive bandwidth selection optic a laser beam comprising a plurality of temporally separated portions of each pulse, each temporally separated portion of each pulse having one of at least two different selected center wavelengths. The tuning mechanism may comprise a plurality of spatial incidence angle selection elements each defining an angle of incidence for a spatially separated but not temporally separated portion of the laser light pulse, and a plurality of temporal angle of incidence selection elements each defining at least a first angle of incidence for at least a first temporally separated portion of each spatially separated but not temporally separated portion of the pulse and a second angle of incidence for a second temporally separated but not spatially separated portion of each spatially separated portion of the pulse.
    • 公开了一种用于在窄带短脉冲持续时间气体放电激光输出光脉冲束产生系统中提供带宽控制的装置和方法,其产生包括选定脉冲重复频率的激光输出光脉冲的光束,其可以包括色散带宽选择光学器件 (图1,字符120)为每个脉冲选择至少一个中心波长,所述至少一个中心波长至少部分地由在分散波长选择光学器件上包含相应脉冲的激光束脉冲光束的入射角度确定;调谐机构, 选择至少一个角度(
    • 7. 发明申请
    • HIGH RESOLUTION SPECTRAL MEASUREMENT DEVICE
    • 高分辨率光谱测量装置
    • WO2003078940A2
    • 2003-09-25
    • PCT/US2003/002052
    • 2003-01-15
    • CYMER, INC.SANDSTROM, Richard, L.ERSHOV, Alexander, I.PARTLO, William, N.FOMENKOV, Igor, V.SMITH, Scott, T.BROWN, Daniel, J., W.
    • SANDSTROM, Richard, L.ERSHOV, Alexander, I.PARTLO, William, N.FOMENKOV, Igor, V.SMITH, Scott, T.BROWN, Daniel, J., W.
    • G01J
    • G01J3/26G01J1/4257G01J3/02G01J3/0205G01J3/12G01J3/1804G01J3/22G01J9/02
    • A high resolution spectral measurement device. A preferred embodiment presents an extremely narrow slit function in the ultraviolet range and is very useful for measuring bandwidth of narrow-band excimer lasers used for integrated circuit lithography. Light from the laser is focused into a diffuser and the diffused light exiting the diffuser illuminates an etalon. A portion of its light exiting the etalon is collected and directed into a slit positioned at a fringe pattern of the etalon. Light passing through the slit is collimated and the collimated light illuminates a grating positioned in an approximately Littrow configuration which disburses the light according to wavelength. A portion of the dispursed light representing the wavelength corresponding to the selected etalon fringe is passed through a second slit and monitored by a light detector. When the etalon and the grating are tuned to the same precise wavelength a slit function is defined which is extremely narrow such as about 0.034pm (FWHM) and about 0.091pm (95 percent integral). The bandwidth of a laser beam can be measured very accurately by a directing portion of the laser beam into the insulator and scanning the laser wavelength over a range which includes the monochromator slit wavelength. In a second embodiment the second slit and the light detector is replaced by a photodiode array and the bandwidth of a laser beam is determined by analyzing a set of scan data from the photodiode array. Alternately, the laser wavelength can be fixed near the middle of the spectrum range of the grating spectrometer, and the etalon can be scanned.
    • 高分辨率光谱测量装置。 优选的实施例在紫外线范围内呈现非常窄的狭缝功能,并且对于测量用于集成电路光刻的窄带准分子激光器的带宽是非常有用的。 来自激光器的光聚焦成漫射器,离散扩散器的散射光照射标准具。 将其从标准具出射的光的一部分收集并引导到位于标准具的边缘图案处的狭缝中。 通过狭缝的光线被准直,并且准直光照射位于大约Littrow配置中的光栅,其根据波长散发光。 表示对应于所选择的标准具条纹的波长的调度光​​的一部分通过第二狭缝并由光检测器监视。 当标准具和光栅调谐到相同的精确波长时,定义了狭缝功能,其极窄,例如约0.034pm(FWHM)和约0.091μm(95%积分)。 通过激光束的引导部分进入绝缘体并且在包括单色器狭缝波长的范围内扫描激光波长,可以非常精确地测量激光束的带宽。 在第二实施例中,第二狭缝和光检测器被光电二极管阵列代替,并且通过分析来自光电二极管阵列的一组扫描数据来确定激光束的带宽。 或者,激光波长可以固定在光栅光谱仪的光谱范围附近,可以扫描标准具。
    • 8. 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。