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    • 1. 发明申请
    • SPATIALLY RELAYING RADIATION COMPONENTS
    • 空间继电器辐射组件
    • WO2012139744A1
    • 2012-10-18
    • PCT/EP2012/001541
    • 2012-04-05
    • MAX-PLANCK-GESELLSCHAFT ZUR FÖRDERUNG DER WISSENSCHAFTEN E. V.LUDWIG-MAXIMILIANS-UNIVERSITÄT MÜNCHENPRONIN, OlegAPOLONSKIY, AlexanderKRAUSZ, FerencPERVAK, Vladimir
    • PRONIN, OlegAPOLONSKIY, AlexanderKRAUSZ, FerencPERVAK, Vladimir
    • G02B27/14G03F7/20G02B5/28H01S3/00
    • G02B27/1006G01N21/25G02B5/283H01S3/08H01S3/08059H01S3/106
    • A method of spatially relaying a first radiation component (1) having a first wavelength and a second radiation component (2) having a second wavelength different from the first radiation component (1), using an optical relaying device (10) which comprises a transparent plate (11) having anti-reflection coatings (12, 13) on both side surfaces thereof, comprises transmitting the first radiation component (1) across the optical relaying device (10) with predetermined incident (a) and emergent angles (β), resp., wherein said anti-reflection coatings (12, 13) being effective for the first radiation component (1) at the incident and emergent angles (α, β), resp., and reflecting the second radiation component (2) at the optical relaying device (10) with a predetermined reflection angle (a) being equal to at least one of said incident and emergent angles (α, β), wherein the first and second radiation components (1, 2) are split from each other toward different directions or combined into a common beam path. Furthermore, an optical relaying device (10) and a resonator device, in particular enhancement cavity device (100) and a laser resonator, are described.
    • 一种使用包括透明的光中继装置(10)的具有第一波长的第一辐射分量(1)和具有不同于第一辐射分量(1)的第二波长的第二辐射分量(2)的空间中继的方法, 在其两个侧表面上具有抗反射涂层(12,13)的板(11)包括以预定入射(a)和出射角(β)穿过光中继装置(10)传输第一辐射分量(1) 其中所述防反射涂层(12,13)在入射和出射角度(a,β)处对第一辐射部件(1)有效,并且在第二辐射部件(2)处于 光学中继装置(10)具有等于所述入射角和出射角(a,β)中的至少一个的预定反射角(a),其中所述第一和第二辐射分量(1,2)彼此分开朝向 不同的方向或组合成一个 公共光束路径。 此外,描述了光中继装置(10)和谐振器装置,特别是增强型腔装置(100)和激光谐振器。
    • 4. 发明申请
    • PULSE LIGHT SOURCE DEVICE AND METHOD FOR CREATING CEP STABLE FS LASER PULSES
    • 脉冲光源装置和用于制造CEP稳定的FS激光脉冲的方法
    • WO2017211374A1
    • 2017-12-14
    • PCT/EP2016/000965
    • 2016-06-10
    • MAX-PLANCK-GESELLSCHAFT ZUR FÖRDERUNG DER WISSENSCHAFTEN E. V.LUDWIG-MAXIMILIANS-UNIVERSITÄT MÜNCHEN
    • KRAUSZ, FerencFATTAHI, Hanieh
    • H01S3/00H01S3/13H01S3/23G02F1/39
    • A pulse light source device (100) for creating fs output laser pulses (1, 1.1, 1.2, 1.3) having CEP stability comprises a pulse source device (10) creating primary ps laser pulses, a first beam splitting device (13) splitting the primary ps laser pulses to first ps laser pulses (2.1) and second ps laser pulses (2.2), a pulse shortening device (20) creating sub-ps laser pulses (3) by shortening and spectrally broadening the first ps laser pulses (2.1), a primary supercontinuum generation device (30) creating primary fs laser pulses (4), a pulse stretcher device (40) creating stretched ps laser pulses (5, 5.1) by stretching the primary fs laser pulses (4), a optical parametric chirped-pulse amplification device (51) creating amplified ps laser pulses (6, 6.1) on the basis of the stretched ps laser pulses (5, 5.1) and the second ps laser pulses (2.2); a phase stabilization device (61) creating CEP stable ps laser pulses (7, 7.1) by difference frequency generation of the amplified ps laser pulses (6, 6.1) and reference laser pulses derived from the primary ps laser pulses (2) or the sub-ps laser pulses (3), a pulse compressor device (71) creating compressed fs laser pulses (8, 8.1) by compressing the CEP stable ps laser pulses (7, 7.1) output by the phase stabilization device (61), and a secondary supercontinuum generation device (81) creating fs output laser pulses as the fs output laser pulses (1, 1.1) to be obtained by spectrally broadening the compressed fs laser pulses (8, 8.1). Furthermore, a method of creating fs output laser pulses is described.
    • 用于产生具有CEP稳定性的fs输出激光脉冲(1,1.1,1.2,1.3)的脉冲光源装置(100)包括产生主ps激光脉冲的脉冲源装置(10),第一 (2.1)和第二ps激光脉冲(2.2),通过缩短和光谱加宽产生亚ps激光脉冲(3)的脉冲缩短装置(20),所述分束装置(13)将所述主ps激光脉冲分为第一ps激光脉冲 第一ps激光脉冲(2.1),产生初级fs激光脉冲(4)的主超连续光谱产生装置(30),通过拉伸初级fs激光脉冲(4)产生拉伸ps激光脉冲(5,5.1)的脉冲展宽器装置 (5)和第二ps激光脉冲(2.2)的基础上产生放大的ps激光脉冲(6,6.1)的光学参量啁啾脉冲放大装置(51)。 通过由放大的ps激光脉冲(6,6.1)和由主ps激光脉冲(2)或子激光脉冲(2)得到的参考激光脉冲的差频产生CEP稳定的ps激光脉冲(7,7.1)的相位稳定装置(61) - 激光脉冲(3); - 脉冲压缩器装置(71),通过压缩由相位稳定装置(61)输出的CEP稳定的ps激光脉冲(7,7.1)产生压缩的fs激光脉冲(8,8.1) 次级超连续谱产生装置(81)产生fs输出激光脉冲作为fs输出激光脉冲(1,1.1),通过对压缩的fs激光脉冲(8,8.1)进行光谱展宽而获得。 此外,还介绍了一种创建fs输出激光脉冲的方法。
    • 10. 发明申请
    • METHOD AND DEVICE FOR CAVITY-ENHANCED BROADBAND INTRAPULSE DIFFERENCE FREQUENCY GENERATION
    • 加速宽带宽带差分频率生成的方法和装置
    • WO2016029981A1
    • 2016-03-03
    • PCT/EP2015/001437
    • 2015-07-13
    • LUDWIG-MAXIMILIANS- UNIVERSITÄT MÜNCHENMAX-PLANCK-GESELLSCHAFT ZUR FÖRDERUNG DER WISSENSCHAFTEN E. V.
    • APOLONSKIY, AlexanderFILL, ErnstPUPEZA, IoachimKRAUSZ, Ferenc
    • G02F1/35
    • G02F1/3534G02F1/3501G02F2001/3503G02F2001/3507G02F2001/3542G02F2203/15
    • A method of creating difference frequency (DF) laser pulses (1) by difference frequency generation (DFG) comprises the steps of providing ultrashort laser pulses (2) having a spectral bandwidth corresponding to a Fourier limit of below 50fs and containing first spectral components and second spectral components having larger frequencies than the first spectral components, and driving a DFG process by the ultrashort laser pulses (2) in an optically non-linear crystal (10), wherein the DF laser pulses (1) are generated in the crystal (10) by difference frequencies between the first and second spectral components, resp., said difference frequencies comprising third spectral components being lower in frequency than the first and second spectral components, wherein at least one enhancement cavity (20) with resonator mirrors (Mil to Ml4) spanning a beam path (22) is provided and the crystal (10) is placed in the beam path (22) of the enhancement cavity (20), the ultrashort laser pulses (2) are input coupled and coherently added in the at least one enhancement cavity (20), at least one circulating ultrashort laser pulse (3) is created in the at least one enhancement cavity (20), which drives the DFG process in the crystal (10) for generating the DF laser pulses (1), and the at least one enhancement cavity (20) is adapted for recycling the at least one ultrashort laser pulse (3) passing through the crystal (10). Furthermore, a photonic source (100) for creating DF laser pulses (1) is described, including one or more enhancement cavities.
    • 通过差频产生(DFG)产生差分频率(DF)激光脉冲(1)的方法包括以下步骤:提供超短激光脉冲(2),其具有对应于低于50fs的傅立叶极限的谱带宽并且包含第一光谱分量, 第二光谱分量具有比第一光谱分量更大的频率,以及通过在非线性晶体(10)中的超短激光脉冲(2)驱动DFG处理,其中DF激光脉冲(1)在晶体中产生 10)由第一和第二光谱分量之间的差频率分配,包括第三光谱分量的所述差分频率在频率上低于第一和第二光谱分量,其中至少一个具有谐振器反射镜的增强空腔(20) 提供跨越光束路径(22)的Ml4,并且晶体(10)被放置在增强腔(20)的光束路径(22)中,超短激光脉冲(2)a 在所述至少一个增强空腔(20)中耦合并相干地添加至少一个增强空腔(20)中的至少一个循环超短激光脉冲(3),其在所述至少一个增强空腔(20)中产生,其驱动所述晶体 ),并且所述至少一个增强腔(20)适于再循环通过所述晶体(10)的所述至少一个超短激光脉冲(3)。 此外,描述了用于产生DF激光脉冲(1)的光子源(100),包括一个或多个增强腔。