首页> 外文会议>Conference on X-Ray Mirrors, Crystals, and Multilayers II; Jul 10-11, 2002; Seattle, Washington, USA >Design and performance of the flexural hinge-based mirror bender at the SLS protein crystallography beamline X06SA
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Design and performance of the flexural hinge-based mirror bender at the SLS protein crystallography beamline X06SA

机译:SLS蛋白结晶学线X06SA上基于弯曲铰链的镜面弯曲器的设计和性能

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The mirror bender installed at the SLS protein crystallography beamline is designed to be capable of adjusting the vertical phase space of the undulator to the acceptance of protein crystals, i.e. to produce micro-beams as well as essentially parallel beams. The two-moment bender is based on the flexural hinge design pioneered at the ESRF but adapted to high-vacuum by making use of in-vacuum motors and high resolution worm-gears. Special care was taken in the design and fabrication of the clamps and the application of the clamping torque. The Rh-coated fused silica substrate (Zeiss) has a free length of 400 mm and a thickness of 30 mm. Metrology tests at ESRF indicate the high quality of the mirror and the bender. Over the useful length of 350 mm the meridional slope error was found to be 0.17-0.3 μrad (rms) prior to, and less than 0.5 μrad after clamping to the bender. In practice this allows the full central cone of an in-vacuum undulator to be focussed to 7 μm at an image distance of 7.1 m and to 2.1 μm at 1.75 m, corresponding to effective slope errors of less than 0.25 μrad. The bending is very reproducible and is well described by an interaction matrix. Finally, the long range tails were measured in the context of the generation of f s-pulses by means of bunch slicing. Their level cannot be attributed to the surface roughness of 2.9 A (rms) but rather to scattering from other beamline components such as Be-win-dows.
机译:安装在SLS蛋白质晶体学生产线上的镜面弯曲器设计为能够调节波状起伏器的垂直相空间以适应蛋白质晶体的接收,即产生微束以及基本平行的光束。这种两片式弯管机基于在ESRF上首创的挠性铰链设计,但通过使用真空马达和高分辨率蜗轮蜗杆而适用于高真空。在设计和制造夹具以及施加夹紧扭矩时要格外小心。涂有Rh的熔融石英基板(蔡司)的自由长度为400毫米,厚度为30毫米。 ESRF的计量测试表明反射镜和弯曲机的质量很高。在350 mm的有效长度上,子午线斜率误差在夹紧弯管机之前为0.17-0.3μrad(rms),而在夹紧弯管机后小于0.5μrad。在实践中,这允许真空内波动器的整个中心锥在7.1 m的像距处聚焦到7μm,在1.75 m的聚焦处聚焦到2.1μm,这对应于小于0.25μrad的有效斜率误差。弯曲是非常可复制的,并且可以通过交互矩阵很好地描述。最后,通过束切在产生f s脉冲的情况下测量了长尾巴。它们的水平不能归因于2.9 A(rms)的表面粗糙度,而是归因于其他光束线组件(例如Be-win-dows)的散射。

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