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
    • 93. 发明申请
    • Laser system
    • 激光系统
    • US20080267241A1
    • 2008-10-30
    • US11982152
    • 2007-10-31
    • Daniel J.W. BrownWilliam N. PartloRichard L. Sandstrom
    • Daniel J.W. BrownWilliam N. PartloRichard L. Sandstrom
    • H01S3/22
    • H01S3/2308G03F7/70025G03F7/70041G03F7/7055G03F7/70575G03F7/70583H01S3/005H01S3/0057H01S3/08036H01S3/225H01S3/2325H01S3/2383
    • An apparatus/method which may comprise: a very high power line narrowed lithography laser light source which may comprise: a solid state seed laser system which may comprise: a pre-seed laser providing a pre-seed laser output; a fiber amplifier receiving the pre-seed laser output and providing an amplified seed laser pulse which may comprise: a pulse having a nominal wavelength outside of the DUV range; a frequency converter converting to essentially the wavelength of the amplifier gain medium; a first and a second gas discharge laser amplifier gain medium operating at different repetition rates from that of the seed laser output; a beam divider providing the amplifier gain mediums with output pulses from the seed laser; a beam combiner combining the outputs of each respective amplifier gain medium to provide a laser output light pulse beam having the pulse repetition rate of the solid state seed laser system.
    • 可以包括:非常高的电力线狭窄的光刻激光光源,其可以包括:固态种子激光系统,其可以包括:提供种子间激光输出的种子间激光; 接收所述种子间激光输出并提供放大的种子激光脉冲的光纤放大器,其可以包括:具有在所述DUV范围之外的标称波长的脉冲; 变换器基本上转换为放大器增益介质的波长; 第一和第二气体放电激光放大器增益介质,与种子激光输出的重复频率不同; 一个分束器,为放大器增益介质提供来自种子激光器的输出脉冲; 组合各个放大器增益介质的输出的光束组合器,以提供具有固态种子激光器系统的脉冲重复率的激光输出光脉冲光束。
    • 95. 发明授权
    • Line narrowing module
    • US07366219B2
    • 2008-04-29
    • US11000684
    • 2004-11-30
    • J. Martin AlgotsRobert A. BergstedtWalter D. GillespieVladimir A. KulgeykoWilliam N. PartloGerman E. RylovRichard L. SandstromBrian StrateTimothy S. Dyer
    • J. Martin AlgotsRobert A. BergstedtWalter D. GillespieVladimir A. KulgeykoWilliam N. PartloGerman E. RylovRichard L. SandstromBrian StrateTimothy S. Dyer
    • H01S3/22
    • H01S3/1055G03F7/70025G03F7/70041H01S3/005H01S3/036H01S3/08H01S3/08004H01S3/08059H01S3/097H01S3/106H01S3/2251
    • A line narrowing method and module for a narrow band DUV high power high repetition rate gas discharge laser producing output laser light pulse beam pulses in bursts of pulses, the module having a nominal optical path are disclosed which may comprise: a dispersive center wavelength selection optic moveably mounted within an optical path of the line narrowing module, 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 first tuning mechanism operative in part to select the angle of incidence of the laser light pulse beam containing the respective pulse upon the dispersive center wavelength selection optic, by selecting an angle of transmission of the laser light pulse beam containing the pulse toward the dispersive center wavelength selection optic; a second tuning mechanism operative in part to select the angle of incidence of the laser light pulse beam containing the respective pulse by changing the position of the dispersive center wavelength selection optic relative to the nominal optical path of the line narrowing module; wherein the second tuning mechanism coarsely selects a value for the center wavelength and the first tuning mechanism more finely selects the value for the center wavelength. The apparatus and method may further comprise at least one beam expanding and redirecting prism in the optical path of the line narrowing module; the first tuning mechanism selecting an angle of incidence of the at least a first spatially defined portion of the laser light pulse beam by changing the position of the at least one beam expanding prism relative to the nominal optical path of the line narrowing module. The first and second tuning mechanisms may be controlled by a center wavelength controller during a burst based upon feedback from a center wavelength detector detecting the center wavelength of at least one other pulse in the burst of pulses and the controller providing the feedback based upon an algorithm employing the detected center wavelength for the at least one other pulse in the burst. The first tuning mechanism may comprise an electro-mechanical course positioning mechanism and a fine positioning mechanism comprising an actuatable material that changes position or shape when actuated.
    • 97. 发明授权
    • Electric discharge laser with active wavelength chirp correction
    • 具有有源波长啁啾校正的放电激光器
    • US06621846B1
    • 2003-09-16
    • US09501160
    • 2000-02-09
    • Richard L. SandstromPalash P. DasGeorge J. EverageFrederick G. ErieWilliam N. PartloIgor V. Fomenkov
    • Richard L. SandstromPalash P. DasGeorge J. EverageFrederick G. ErieWilliam N. PartloIgor V. Fomenkov
    • H01S322
    • H01S3/104G03F7/70025G03F7/70333G03F7/70575G03F7/708H01S3/036H01S3/038H01S3/0381H01S3/0382H01S3/105H01S3/1055H01S3/13H01S3/134H01S3/225
    • Electric discharge laser with active chirp correction. This application discloses techniques for moderating and dispensing these pressure waves. In some lasers small predictable patterns remain which can be substantially corrected with active wavelength control using relatively slow wavelength control instruments of the prior art. In a preferred embodiment a simple learning algorithm is described to allow advance tuning mirror adjustment in anticipation of the learned chirp pattern. Embodiments include stepper motors having very fine adjustments so that size of tuning steps are substantially reduced for more precise tuning. However, complete elimination of wavelength chirp is normally not feasible with structural changes in the laser chamber and advance tuning; therefore, Applicants have developed equipment and techniques for very fast active chirp correction. Improved techniques include a combination of a relatively slow stepper motor and a very fast piezoelectric driver. In another preferred embodiment chirp correction is made on a pulse-to-pulse basis where the wavelength of one pulse is measured and the wavelength of the next pulse is corrected based on the measurement. This correction technique is able to function at repetition rates as rapid as 2000 Hz and greater.
    • 具有主动啁啾校正的放电激光器。 本申请公开了用于调节和分配这些压力波的技术。 在一些激光器中,可以使用现有技术的相对较慢的波长控制装置的主动波长控制基本上校正了小的可预测的图案。 在优选实施例中,描述了一种简单的学习算法,以便在预期学习的啁啾模式中允许预调谐镜调节。 实施例包括具有非常精细调节的步进电动机,使得调节步骤的尺寸被显着减小以便更精确的调谐。 然而,完全消除波长啁啾通常不可行,在激光室的结构变化和提前调谐; 因此,申请人已经开发了用于非常快的主动啁啾校正的设备和技术。 改进的技术包括相对较慢的步进电机和非常快的压电驱动器的组合。 在另一个优选实施例中,在脉冲对脉冲基础上进行啁啾校正,其中测量一个脉冲的波长,并且基于测量校正下一个脉冲的波长。 该校正技术能够以2000Hz及更高​​的重复速率工作。
    • 98. 发明授权
    • High resolution etalon-grating monochromator
    • 高分辨率标准光栅单色仪
    • US06480275B2
    • 2002-11-12
    • US09772293
    • 2001-01-29
    • Richard L. SandstromAlexander I. ErshovWilliam N. PartloIgor V. FomenkovScott T. Smith
    • Richard L. SandstromAlexander I. ErshovWilliam N. PartloIgor V. FomenkovScott T. Smith
    • G01J318
    • G01J3/12G01J1/4257G01J3/22G01J3/26G01J9/02
    • A high resolution etalon-grating monochromator. 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 0.034 pm (FWHM) and about 0.091 pm (95 percent integral). The bandwidth of a laser beam can be measured very accurately by a directing portion of the laser beam into the monochromator and scanning the laser wavelength over a range which includes the monochromator slit wavelength.
    • 高分辨率标准光栅单色仪。 优选的实施例在紫外范围内呈现非常狭窄的狭缝功能,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。 来自激光的光被聚焦成漫射器,并且离开扩散器的漫射光照射标准具。 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,定义狭缝功能,其极窄,例如约0.034μm(FWHM)和约0.091μm(95%积分)。 激光束的带宽可以通过激光束的引导部分进入单色仪并且在包括单色器狭缝波长的范围内扫描激光波长而被非常精确地测量。