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    • 2. 发明申请
    • CHIRPED DICHROIC MIRROR AND A SOURCE FOR BROADBAND LIGHT PULSES
    • US20150229093A1
    • 2015-08-13
    • US14622555
    • 2015-02-13
    • Deutsches Elektronen-Synchrotron DESY
    • Franz KärtnerShih-Hsuan Chia
    • H01S3/00G02B5/08
    • H01S3/0057G02B5/0816G02B5/0825G02B5/281G02B27/1006G02B27/141H01S3/2391
    • The present invention is directed to a chirped dichroic mirror comprising a stack of alternating high refractive index and low refractive index layers, a front end portion including an antireflective coating followed by an impedance matching region in which the ratio of the optical thickness of a high refractive index layer to the optical thickness of the next following low refractive index layer is adiabatically increasing to a first value, the impedance matching region being followed by a chirped mirror region where the Bragg wavelength of the layer pair is generally increasing or generally decreasing, characterized in that the layers in a back end region form a second impedance matching region in which the ratio of the optical thickness of a high refractive index layer to the optical thickness of the next following low refractive index layer starts at the value of this ratio in the adjacent chirped mirror region and is then adiabatically decreasing in order to provide matched impedance to the surrounding medium over the transmission spectral band.
    • 本发明涉及一种啁啾分光镜,其包括交替的高折射率和低折射率层的叠层,前端部分包括抗反射涂层,其后是阻抗匹配区域,其中高折射率和高折射率层的光学厚度的比率 索引层与下一个低折射率层的光学厚度绝热地增加到第一值,阻抗匹配区域后面是啁啾反射镜区域,其中层对的布拉格波长通常增加或通常减小,其特征在于 后端区域中的层形成第二阻抗匹配区域,其中高折射率层的光学厚度与下一个低折射率层的光学厚度的比率以相邻的该比率的该值的值开始 啁啾镜区域,然后绝热地减少以提供匹配的障碍 通过传输光谱带向周围介质传播。
    • 4. 发明申请
    • METHOD FOR PRODUCING A MULTILAYER LAUE LENS
    • US20220146721A1
    • 2022-05-12
    • US17453433
    • 2021-11-03
    • Deutsches Elektronen-Synchrotron DESY
    • Henry ChapmanSasa BajtMauro Prasciolu
    • G02B5/18G21K1/06
    • Disclosed is a method for producing a multilayer Laue lens. The object to provide a method for producing a wedged MLL that can be operated over a large range of wavelengths, and which preferably requires only a linear stage to adjust the positions of the lens as the wavelength is changed, is achieved by providing a lens blank comprising a substrate element having a flat upper surface extending in a plane defined by orthogonal axes x, y, z, wherein x and z extend in the plane and y extends normal to the plane, a layered structure deposited on the upper surface of the substrate element in such a way that at least two different materials are layered upon one another in an alternating manner, wherein the y-extension of the layered structure is constant along the x-axis and varies along the z-axis within a ramp section where the y-extension of the layered structure increases from a starting point, where first particles of material of the layered structure are deposited on the upper surface of the substrate element, to a saturation point, where a maximum y-extension of the layered structure is reached; and slicing a lens out of the lens blank by slicing through the ramp section in parallel to the y-axis but not parallel to the x- and z-axes.
    • 8. 发明申请
    • X-RAY PULSE SOURCE AND METHOD FOR GENERATING X-RAY PULSES
    • X射线脉冲源和产生X射线脉冲的方法
    • US20160323985A1
    • 2016-11-03
    • US15050514
    • 2016-02-23
    • Deutsches Elektronen-Synchrotron DESY
    • Franz X. KAERTNERArya FALLAHI
    • H05G2/00
    • H05G2/008H01S3/0903H05G2/00H05H9/02H05H2007/027H05H2007/041
    • X-ray pulse source (100) for generating X-ray pulses (1) includes electron pulse source device (10) including photo-emitter device (11) being configured for photo-induced creation of free electron pulses (2) and driver device (12) being configured for creating electromagnetic driver pulses (3) accelerating electron pulses (2) along acceleration path (7), and electromagnetic interaction device (50) comprising electromagnetic pulse source device (51) being configured for creating electromagnetic pulses (4) in interaction section (5) of electromagnetic interaction device (50), wherein electron pulse source device (10) and electromagnetic interaction device (50) are operable for generating X-ray pulses (1) by an interaction of electron pulses (2) and electromagnetic pulses (4), and driver device (12) includes THz driver pulse source (13), which is configured for creating single cycle or multi cycle THz driver pulses (3). Furthermore, a method of creating X-ray pulses (1) is described.
    • 用于产生X射线脉冲(1)的X射线脉冲源(100)包括电子脉冲源装置(10),其包括被配置用于光致产生自由电子脉冲(2)的光发射器件(11)和驱动器装置 (12)被配置为用于产生沿着加速路径(7)加速电子脉冲(2)的电磁驱动器脉冲(3);以及电磁相互作用装置(50),包括被配置用于产生电磁脉冲(4)的电磁脉冲源装置(51) 在电磁相互作用装置(50)的相互作用部分(5)中,电子脉冲源装置(10)和电磁相互作用装置(50)可用于通过电子脉冲(2)和 电磁脉冲(4)和驱动器装置(12)包括被配置用于产生单周期或多周期THz驱动脉冲(3)的THz驱动脉冲源(13)。 此外,描述了创建X射线脉冲(1)的方法。
    • 10. 发明申请
    • Device and Method for Characterizing an Ultrashort Laser Pulse
    • 用于表征超短脉冲激光脉冲的装置和方法
    • US20160116338A1
    • 2016-04-28
    • US14920260
    • 2015-10-22
    • Deutsches Elektronen-Synchrotron DESY
    • Matthew STREETERJens OSTERHOFF
    • G01J3/457G01J3/02H01S3/00
    • G01J3/457G01J3/0205G01J11/00H01S3/0014H01S3/005H01S3/0092
    • The invention relates to a device (2) and to a method for characterizing an ultrashort laser pulse. Furthermore, the invention relates to use of a self-contained optical assembly in a device (2) for characterizing an ultrashort laser pulse. The device (2) comprises an imaging optical element (4) configured to image the incident laser pulse (6) in a direction of a straight line (L). A first optical element (10) is configured to apply predetermined varying group delay dispersion on the line focused laser pulse. A non-linear optical element (14) is configured to generate a second harmonic laser pulse (30). An optical grating (20) generates a diffraction of the second harmonic laser pulse, which is imaged on a flat sensor (24). A processing unit (36) determines a best fit for the captured image thereby calculating a frequency spectrum and a spectral phase of the laser pulse.
    • 本发明涉及一种用于表征超短激光脉冲的装置(2)和方法。 此外,本发明涉及在用于表征超短激光脉冲的装置(2)中使用独立的光学组件。 装置(2)包括成像光学元件(4),被配置为沿着直线(L)的方向成像入射激光脉冲(6)。 第一光学元件(10)被配置为在线聚焦激光脉冲上施加预定的变化组延迟色散。 非线性光学元件(14)被配置为产生二次谐波激光脉冲(30)。 光栅(20)产生成像在平面传感器(24)上的二次谐波激光脉冲的衍射。 处理单元(36)确定捕获图像的最佳拟合,从而计算激光脉冲的频谱和频谱相位。