同步辐射有源波束衰减器

J. Hasi, C. Kenney, C. Da Via, S. Parker, A. Thompson, E. Westbrook
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引用次数: 2

摘要

在同步加速器束流线上使用衰减材料来实现光子通量调制和x射线光谱的束流硬化。在一些实验中,当同步加速器中的电流在填充周期内衰减时,希望将光束在样品上的强度保持在恒定值。这通常是通过用一组离散的薄箔来衰减入射光束来完成的。要改变光束路径中的材料量,通常需要插入或重新绘制一些箔片。离散箔的使用对可用厚度值的数量以及最小厚度增量施加了实际限制。微机械衰减器可以通过提供材料厚度的连续变化或通过实施大量小厚度步骤来避免这些限制。通过光刻和适当的器件几何结构相结合,可以制造亚微米厚度增量。器件几何形状,如楼梯,低角三角形和重叠三角形将被描述。通过对材料(如硅)的直接微加工以及各种聚合物的微成型,可以相对容易地制造这些器件。此外,通过在衰减器中制造一个硅二极管,可以连续监测光束的吸收部分。通过使用一个反馈回路,其中衰减器的厚度是根据下游光束监视器变化的,它应该有可能保持样品上的光子通量变化小于0.5%。介绍了各种器件在先进光源下的性能。
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Active beam attenuators for synchrotron radiation
Attenuating materials are employed on synchrotron beam lines to achieve photon flux modulation as well as beam hardening of the x-ray spectrum. In some experiments it is desirable to maintain the intensity of the beam on the sample at a constant value as the current in the synchrotron decays during a fill cycle. This is often done by attenuating the incident beam with a set of discrete, thin foils. To change the amount of material in the beam path typically involves inserting or redrawing a number of foils. The use of discrete foils imposes practical limits on the number of thickness values available as well as the smallest thickness increment. Micro-machined attenuators can avoid these restrictions by offering either continuous variation of the material thickness or through the implementation of a large number of small thickness steps. Through a combination of photolithography and appropriate device geometry sub-micron thickness increments can be fabricated. Device geometries such as staircase, low-angle triangle, and overlapping triangles will be described. Fabrication of these devices by direct micro-machining of materials such as silicon as well as micro-molding of various polymers can be done relatively easily. In addition, by manufacturing a silicon diode into the attenuator the absorbed fraction of the beam can be continuously monitored. By using a feedback loop where the attenuator thickness is varied based on a downstream beam monitor, it should be possible to maintain the photon flux on a sample to vary by less than 0.5%. The performance of a variety of these devices at the Advanced Light Source is presented.
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