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MOPMR054 |
Double-slit Interferometer Measurements at SPEAR3 |
368 |
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- C.L. Li, W.J. Zhang
East China University of Science and Technology, Shanghai, People's Republic of China
- M.J. Boland
SLSA, Clayton, Australia
- W.J. Corbett, M. Grinberg
SLAC, Menlo Park, California, USA
- T.M. Mitsuhashi
KEK, Ibaraki, Japan
- Y.H. Xu
DongHua University, Songjiang, People's Republic of China
- W.J. Zhang
University of Saskatchewan, Saskatoon, Canada
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The resolution of a conventional telescope used to image visible-light synchrotron radiation is often limited by diffraction effects. To improve resolution, the double-slit interferometer method was developed at KEK and has since become popular around the world. Based on the Van Cittert-Zernike theorem relating transverse source profile to transverse spatial coherence, the particle beam size can be inferred by recording fringe contrast as a function of interferometer slit separation. In this paper, we describe the SPEAR3 double-slit interferometer, develop a theoretical framework for the interferometer and provide experimental results. Of note the double-slit system is 'rotated' about the beam axis to map the dependence of photon beam coherence on angle.
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THPOY050 |
Time Response of a Gridded X-ray Beam Ionization Chamber |
4220 |
SUPSS083 |
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- Y.H. Xu, Z.H. Sun
DongHua University, Songjiang, People's Republic of China
- D.V. Campen, W.J. Corbett
SLAC, Menlo Park, California, USA
- C.L. Li
East China University of Science and Technology, Shanghai, People's Republic of China
- W.J. Zhang
University of Saskatchewan, Saskatoon, Canada
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Recently, Quick-Scanning Extended X-ray Absorption Spectroscopy (QEXAS) has become an important tool for in-situ characterization of materials and measurement of associated electronic structure. In this case the time response of the ionization chamber affects the measurement resolution and therefore overall performance of the QEXAS system. Common parallel-plate ionization chambers have a step-response rise time of about 0.1 sec, which does not meet the requirements of QEXAS. To speed up the response, we constructed a gridded ionization chamber with variable bias voltage and optional background gas (N2 or He, respectively). To characterize the system we used a high-frequency beam chopper upstream of the ionization chamber and a high-speed, low-noise preamplifier to measure the step response of the chamber as a function of bias voltage and background gas conditions.
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