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    • 112. 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。
    • 113. 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。
    • 114. 发明授权
    • Electric discharge laser with acoustic chirp correction
    • 具有声啁啾校正的放电激光器
    • US06317447B1
    • 2001-11-13
    • US09490835
    • 2000-01-25
    • William N. PartloIgor V. FomenkovJean-Marc HueberZsolt BorEckehard D. OnkelsMichael C. CatesRichard C. UjazdowskiVladimir B. FleurovDmitri V. Gaidarenko
    • William N. PartloIgor V. FomenkovJean-Marc HueberZsolt BorEckehard D. OnkelsMichael C. CatesRichard C. UjazdowskiVladimir B. FleurovDmitri V. Gaidarenko
    • H01S322
    • G03F7/70025G03F7/70575G03F7/708H01S3/036H01S3/038H01S3/0381H01S3/0382
    • Methods and structural changes in gas discharge lasers for minimizing wavelength chirp at high pulse rates. Applicants have identified the major cause of wavelength chirp in high pulse rate gas discharge lithography lasers as pressure waves from a discharge reflecting back to the discharge region coincident with a subsequent discharge. The timing of the arrival of the pressure wave is determined by the temperature of the laser gas through which the wave is traveling. During burst mode operation, the laser gas temperature in prior art lasers changes by several degrees over periods of a few milliseconds. These changing temperatures change the location of the coincident pressure waves from pulse to pulse within the discharge region causing a variation in the pressure of the laser gas which in turn affects the index of refraction of the discharge region causing the laser beam exiting the rear of the laser to slightly change direction. This change in beam direction causes the grating in the LNP to reflect back to the discharge region light at a slightly different wavelength causing the wavelength chirp. Solution to the problem is to include in the laser chamber structural elements to moderate or disperse the pressure waves and to maintain the laser gas temperature as close as feasible to constant values.
    • 气体放电激光器的方法和结构变化,以最大限度地减少高脉冲波长啁啾。 申请人已经确定了在高脉冲气体放电光刻激光器中的波长啁啾的主要原因,因为从反射回到放电区域的放电的压力波与随后的放电一致。 压力波的到达时间由波浪行进的激光气体的温度决定。 在突发模式操作期间,现有技术的激光器中的激光气体温度在几毫秒的时间内改变了几度。 这些变化的温度改变了放电区域内重合压力波从脉冲到脉冲的位置,导致激光气体的压力变化,这反过来影响放电区域的折射率,导致激光束离开 激光稍微改变方向。 光束方向的这种变化导致LNP中的光栅以稍微不同的波长反射回到放电区域,导致波长啁啾。 解决问题的方法是在激光室结构元件中包括中压或分散压力波,并将激光气体温度保持在尽可能接近的恒定值。