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    • 1. 发明授权
    • Dielectric coupled CO2 slab laser
    • 介质耦合CO2平板激光器
    • US07260134B2
    • 2007-08-21
    • US10869964
    • 2004-06-17
    • Christian J. ShackletonPhillip J. GardnerAnthony J. DeMariaVernon SeguinJohn T. Kennedy
    • Christian J. ShackletonPhillip J. GardnerAnthony J. DeMariaVernon SeguinJohn T. Kennedy
    • H01S3/22H01S3/097
    • H01S3/2232H01S3/0315H01S3/038H01S3/0385H01S3/0407H01S3/041H01S3/0975
    • An slab CO2 laser includes spaced-apart elongated slab electrodes. A lasing gas fills a discharge gap between the electrodes. An RF power supply is connected across the electrodes and sustains an electrical discharge in the lasing gas in the discharge gap. Either one or two ceramic inserts occupy a portion of width of the electrodes and in contact with the electrodes. A discharge gap is formed between the portions of the width of the electrodes not occupied by the insert or inserts. Provision of the ceramic insert or inserts increases the resistance-capacitance (RC) time constant of the electrode impedance by increasing the capacitive component of the time constant. This hinders the formation of arcs in the discharge, which, in turn enables the inventive laser to operate with higher excitation power or higher lasing-gas pressure than would be possible without the dielectric insert. The ceramic insert also decreases the difference in impedance of the electrodes with and without a discharge. This leads to a better-behaved discharge, and a discharge that is easier to light.
    • 平板CO2激光器包括间隔开的细长板状电极。 激光气体填充电极之间的放电间隙。 RF电源跨越电极连接,并且在放电间隙中的激光气体中保持放电。 一个或两个陶瓷插入件占据电极宽度的一部分并与电极接触。 在未被插入物或插入物占据的电极的宽度部分之间形成放电间隙。 提供陶瓷插件或插件通过增加时间常数的电容分量来增加电极阻抗的电阻 - 电容(RC)时间常数。 这阻碍了放电中的电弧的形成,这又使得本发明的激光器能够在没有电介质插入件的情况下以更高的激发功率或更高的激光气体压力运行。 陶瓷插入件还减少了具有和没有放电的电极的阻抗差异。 这导致更好的放电,并且更容易点亮的放电。
    • 2. 发明授权
    • Dielectric coupled CO2 slab laser
    • 介质耦合CO2平板激光器
    • US07263116B2
    • 2007-08-28
    • US10912507
    • 2004-08-05
    • Christian J. ShackletonPhillip J. GardnerAnthony J. DeMariaVernon SeguinJohn T. Kennedy
    • Christian J. ShackletonPhillip J. GardnerAnthony J. DeMariaVernon SeguinJohn T. Kennedy
    • H01S3/03H01S3/223H01S3/097
    • H01S3/0315H01S3/0388H01S3/0407H01S3/041H01S3/09705H01S3/0971H01S3/2232
    • A slab laser includes two elongated electrodes arranged spaced apart and face-to-face. Either one or two slabs of a solid dielectric material extend along the length of the electrodes between the electrodes. A discharge gap is formed either between one of the electrodes and one dielectric slab, or between two dielectric slabs. The discharge gap is filled with lasing gas. A pair of mirrors is configured and arranged to define a laser resonator extending through the gap. An RF potential is applied across the electrodes creating a gas discharge in the gap, and causing laser radiation to circulate in the resonator. Inserting dielectric material between the electrodes increases the resistance-capacitance (RC) time constant of the discharge structure compared with the RC time constant in the absence of dielectric material. This hinders the formation of arcs in the discharge, which enables the laser to operate with higher excitation power, higher lasing gas pressure, and higher output power than would be possible without the dielectric inserts.
    • 平板激光器包括间隔开并且面对面布置的两个细长电极。 一个或两个固体电介质材料板沿电极的电极长度延伸。 在一个电极和一个电介质板之间或两个电介质板之间形成放电间隙。 放电间隙充满激光气体。 一对反射镜被配置和布置成限定延伸穿过间隙的激光谐振器。 在电极上施加RF电位,在间隙中产生气体放电,并使激光辐射在谐振器中循环。 在不存在电介质材料的情况下,在电极间插入电介质材料会增加放电结构的电阻 - 电容(RC)时间常数。 这阻碍了放电中的电弧形成,这使得激光器能够在没有电介质插入件的情况下以更高的激发功率,更高的激光气体压力和更高的输出功率运行。
    • 6. 发明授权
    • Apparatus for improving the optical intensity induced damage limit of
optical quality crystals
    • 用于改善光学强度的光学质量晶体损伤极限的装置
    • US5680412A
    • 1997-10-21
    • US506782
    • 1995-07-26
    • Anthony J. DeMariaJohn T. KennedyRichard A. Hart
    • Anthony J. DeMariaJohn T. KennedyRichard A. Hart
    • G02F1/35G02F1/355H01S5/024H01S5/10H01S5/16H01S5/50H01S3/08
    • G02F1/3551G02F1/3525H01S3/0092
    • The apparatus of the present invention significantly improves the optical intensity induced damage limit of optical quality crystals, and in particular crystals used in the conversion of laser radiation at a specific wavelength to another wavelength or other wavelengths through non-linear interaction of the input laser radiation with the optical crystal medium. In accordance with the present invention, passive optical elements are positioned at the laser beam exiting and entrance surfaces of the active optical element. The surfaces of the passive optical elements are placed up against respective exiting and entrance surfaces of the active optical element. Since the optically transparent passive optical elements have higher mass than optical coatings, they provide vastly superior cooling, and therefore, considerably higher laser damage threshold for the surfaces. Higher damage thresholds results in a significant increase in the performance, reliability, and failure damage safety margin while reducing size and cost of high intensity laser systems and subsystems that utilize active optical elements.
    • 本发明的装置显着改善了光学质量晶体的光强度诱发的损伤极限,特别是通过输入激光辐射的非线性相互作用将特定波长的激光辐射转换成另一波长或其它波长的晶体 与光学晶体介质。 根据本发明,无源光学元件位于离开激活光学元件的入射表面的激光束处。 无源光学元件的表面被放置在相对于有源光学元件的相应出射和入射表面上。 由于光学透明无源光学元件具有比光学涂层更高的质量,因此它们提供了非常优异的冷却,因此提供了相当高的表面的激光损伤阈值。 更高的损伤阈值导致性能,可靠性和故障损伤安全裕度的显着增加,同时降低了使用有源光学元件的高强度激光系统和子系统的尺寸和成本。
    • 7. 发明授权
    • High power waveguide laser
    • 大功率波导激光器
    • US06788722B1
    • 2004-09-07
    • US09612733
    • 2000-07-10
    • John T. KennedyRichard A. HartLeon A. NewmanAnthony J. DeMaria
    • John T. KennedyRichard A. HartLeon A. NewmanAnthony J. DeMaria
    • H01S322
    • H01S3/0315H01S3/03H01S3/038H01S3/076H01S3/09702H01S3/09705
    • The above discussed and other drawbacks and deficiencies of the prior art are overcome or alleviated by a laser of the present invention. In accordance with the present invention the laser comprises a housing defining a plurality of compartments therein, a folded waveguide disposed within the housing, the folded waveguide defining a plurality of channels having a substantially rectangular cross section for guiding a laser beam, a plurality of electrodes disposed in the plurality of compartments and juxtaposed along opposite surfaces of the waveguide and at least one power supply connected to the plurality of electrodes. The channels having a prescribed width to height ratio for a prescribed channel length for a given Fresnel number. At least one optical housing is provided. The optical housing is mounted to the laser housing, the optical housing including a plurality of beam turning mechanisms disposed within a plurality of compartments accessible for adjusting the beam turning mechanisms. The channels are disposed within the waveguide so as to subtend a prescribed angular orientation between adjacent channels. Inductors are provided for suppressing the capacitance of the electrodes.
    • 现有技术的上述讨论和其它缺陷和不足之处由本发明的激光器克服或减轻。 根据本发明,激光器包括在其中限定多个隔室的壳体,设置在壳体内的折叠波导,折叠波导限定多个通道,其具有用于引导激光束的基本上矩形的横截面,多个电极 设置在所述多个隔室中并且与所述波导的相对表面并置并且连接到所述多个电极的至少一个电源。 对于给定的菲涅耳数,对于规定的通道长度,通道具有规定的宽高比。 提供至少一个光学外壳。 光学壳体安装到激光器壳体上,光学壳体包括多个光束转动机构,其设置在可容纳以调节光束转动机构的多个隔间内。 通道设置在波导内,以便在相邻通道之间对准规定的角度取向。 电感器用于抑制电极的电容。