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    • 3. 发明授权
    • Multiple laser cavity
    • 多激光腔
    • US07260136B2
    • 2007-08-21
    • US10500627
    • 2002-02-22
    • Wolf SteffensUlrich Kallmann
    • Wolf SteffensUlrich Kallmann
    • H01S3/08
    • H01S5/141H01S5/142H01S5/143H01S5/4056H01S5/4087
    • A method of using at least a part of a cavity for a first and at least one second laser includes providing a first laser beam to the part of the cavity, splitting the first beam into a first and a second part, splitting the first part into a third and a fourth part, splitting the second part into a fifth and a sixth part, superimposing the third and the fifth part in a way causing extinguishing interference, superimposing the fourth and the sixth part in a way causing cumulative interference to provide a first resulting beam, and performing the above elements with at least one second laser beam provided to the same part of the cavity to provide a second resulting beam.
    • 使用空腔的至少一部分用于第一和至少一个第二激光的方法包括:将第一激光束提供到空腔的一部分,将第一光束分成第一和第二部分,将第一部分分成 第三部分和第四部分,将第二部分分成第五和第六部分,以导致灭绝干扰的方式叠加第三部分和第五部分,以引起累积干扰的方式叠加第四部分和第六部分,以提供第一部分 并且通过提供到空腔的相同部分的至少一个第二激光束来执行上述元件以提供第二结果光束。
    • 5. 发明申请
    • Cavity with dispersive element
    • 具有色散元件的腔
    • US20060007980A1
    • 2006-01-12
    • US10526168
    • 2002-08-28
    • Jochen SchwarzWolf SteffensUlrich KallmannBernd NebendahlEmmerich Mueller
    • Jochen SchwarzWolf SteffensUlrich KallmannBernd NebendahlEmmerich Mueller
    • H01S3/08H01S3/10
    • H01S3/08036H01S3/08059
    • A laser being tunable in wavelength a first reflecting unit and a second unit, both reflecting units being arranged to at least partially reflect an incident beam of electromagnetic radiation towards each other, an optical path of said beam of electromagnetic radiation within said cavity, which is defined in length by said first and second reflecting unit a dispersive device, which is arranged, such that a portion of said optical path of said beam of electromagnetic radiation traverses through said dispersive device, wherein said dispersive device comprises a dispersive characteristic representing a functional dependence of an optical path length of said portion with respect to wavelength of said electromagnetic 6radiation, wherein said optical path length increases with an increasing wavelength of said electromagnetic radiation.
    • 激光器可以在波长为第一反射单元和第二单元的情况下被调谐,两个反射单元布置成至少部分地将入射的电磁辐射束朝向彼此反射,所述腔内的所述电磁辐射束的光路是 由所述第一和第二反射单元限定分散装置,所述分散装​​置被布置成使得所述电磁辐射束的所述光路的一部分穿过所述分散装​​置,其中所述色散装置包括表示功能依赖性的色散特性 所述部分的光路长度相对于所述电磁辐射的波长,其中所述光程长度随着所述电磁辐射的波长的增加而增加。
    • 6. 发明申请
    • Multiple laser cavity
    • 多激光腔
    • US20050128563A1
    • 2005-06-16
    • US10500627
    • 2002-02-22
    • Wolf SteffensUlrich Kallmann
    • Wolf SteffensUlrich Kallmann
    • H01S5/14H01S5/40G02F1/01
    • H01S5/141H01S5/142H01S5/143H01S5/4056H01S5/4087
    • A method of using at least a part of a cavity for a first and at least one second laser includes providing a first laser beam to the part of the cavity, splitting the first beam into a first and a second part, splitting the first part into a third and a fourth part, splitting the second part into a fifth and a sixth part, superimposing the third and the fifth part in a way causing extinguishing interference, superimposing the fourth and the sixth part in a way causing cumulative interference to provide a first resulting beam, and performing the above elements with at least one second laser beam provided to the same part of the cavity to provide a second resulting beam.
    • 使用空腔的至少一部分用于第一和至少一个第二激光的方法包括:将第一激光束提供到空腔的一部分,将第一光束分成第一和第二部分,将第一部分分成 第三部分和第四部分,将第二部分分成第五和第六部分,以导致灭绝干扰的方式叠加第三部分和第五部分,以引起累积干扰的方式叠加第四部分和第六部分,以提供第一部分 并且通过提供到空腔的相同部分的至少一个第二激光束来执行上述元件以提供第二结果光束。
    • 7. 发明授权
    • Tuning a laser
    • 调整激光
    • US06763044B2
    • 2004-07-13
    • US10159312
    • 2002-05-31
    • Emmerich MuellerRalf HaeusslerWolf SteffensUlrich Kallmann
    • Emmerich MuellerRalf HaeusslerWolf SteffensUlrich Kallmann
    • H01S510
    • H01S5/141H01S3/106H01S3/1066H01S3/1068H01S3/107H01S5/143
    • The invention relates to a method of tuning a laser, comprising the steps of: providing a laser beam to an external cavity, the laser beam traveling through material along a path between a cavity end element and a tuning element, the path having an optical path length, selecting at least one mode of the laser by introducing a dispersion element in the path of the laser, rotating the tuning element about a pivot axis theoretically defined by the intersection of the surface planes of the cavity end element, the dispersion element and the tuning element to tune the laser, changing the optical path length of the path in order to at least partly compensate a shift between the real position of the pivot axis and the theoretically defined position.
    • 本发明涉及一种调谐激光的方法,包括以下步骤:向外腔提供激光束,激光束沿着空腔端元件和调谐元件之间的路径传播通过材料,该路径具有光路 长度,通过在激光的路径中引入色散元素来选择激光的至少一种模式,使调谐元件围绕理论上由空腔端元件,色散元件和色散元件的表面相交界定的枢转轴线旋转 调谐元件以调整激光器,改变路径的光路长度,以便至少部分地补偿枢转轴线的实际位置与理论上定义的位置之间的偏移。
    • 8. 发明授权
    • Wavelength tunable laser with dispersive element
    • 具有色散元件的波长可调谐激光器
    • US07242698B2
    • 2007-07-10
    • US10526168
    • 2002-08-28
    • Jochen SchwarzWolf SteffensUlrich KallmannBernd NebendahlEmmerich Mueller
    • Jochen SchwarzWolf SteffensUlrich KallmannBernd NebendahlEmmerich Mueller
    • H01S3/10H01S3/08
    • H01S3/08036H01S3/08059
    • A laser being tunable in wavelength includes a first reflecting unit and a second reflecting unit, both reflecting units being arranged to at least partially reflect an incident beam of electromagnetic radiation towards each other, an optical path of said beam of electromagnetic radiation within said cavity, which is defined in length by said first and second reflecting unit, a dispersive device, which is arranged, such that a portion of said optical path of said beam of electromagnetic radiation traverses through said dispersive device, wherein said dispersive device comprises a dispersive characteristic representing a functional dependence of an optical path length of said portion with respect to wavelength of said electromagnetic radiation, wherein said optical path length increases with an increasing wavelength of said electromagnetic radiation.
    • 可波长的激光器包括第一反射单元和第二反射单元,两个反射单元布置成至少部分地将入射的电磁辐射束朝向彼此反射,所述腔内的所述电磁辐射束的光路, 其由所述第一和第二反射单元在长度上限定,分散装置被布置成使得所述电磁辐射束的所述光路的一部分穿过所述分散装​​置,其中所述色散装置包括代表 所述部分的光路长度相对于所述电磁辐射的波长的函数依赖性,其中所述光程长度随着所述电磁辐射的波长的增加而增加。