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Polycapillary based μ-XAS and confocal μ-XANES at a bending magnet source of the ESRF

Geert Silversmit et al 2009 J. Phys.: Conf. Ser. 190 012036 (6pp)   doi: 10.1088/1742-6596/190/1/012036  Help

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Geert Silversmit1, Bart Vekemans1, Sergey Nikitenko2, Kristof Tirez3, Wim Bras2, Frank E Brenker4 and Laszlo Vincze1
1 X-ray Microspectroscopy and Imaging Research Group (XMI), Department of Analytical Chemistry, Ghent University, Krijgslaan 281 S12, B-9000 Gent, Belgium
2 Netherlands Organisation for Scientific Research (NWO), DUBBLE at ESRF, BP 220, 38043 Grenoble CEDEX 9, France
3 VITO, Boeretang 200, 2400 Mol, Belgium
4 Geoscience Institute – Mineralogy, Goethe University, Altenhoeferallee 1, 60438 Frankfurt am Main, Germany
E-mail: Geert.Silversmit@UGent.be

Abstract. Glass polycapillary optics are shown to be easy to use focusing optics for bending magnet XAS stations. These achromatic optics have acceptances of several mm horizontally and vertically, while their angular acceptances can be matched to the source divergence by the design of the polycapillary. A polycapillary half-lens based focusing system was successfully tested for transmission and fluorescence μ-XAS at the DUBBLE beamline (BM26A, ESRF) and the feasibility of confocal μ-XANES in fluorescence mode is presented.

Transmission efficiencies of 25–45% with flux density gain factors of about 2000 and beam sizes of 10–20 μm were obtained in the 7–14 keV energy range. Although the polycapillary optic has a smoothly changing energy dependent transmission efficiency, the amplitude and shape of the EXAFS oscillations are not influenced by this. The focusing properties of the polycapillary lens cancel slight vertical motions of the incoming X-ray beam, resulting in a fixed μ-beam spot in the focal plane, making polycapillaries also suitable optic in combination with a non-fixed exit monochromator.

In addition, by mounting a second polycapillary half-lens in front of an energy dispersive detector, a confocal set-up is obtained, which restricts the part of the sample seen by the detector to a microscopic volume of about 20×20×15 μm3 at the Fe K absorption edge for example.

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