D3, the new diffractometer for the macromolecular crystallography beamlines of the Swiss Light Source

Fuchs, M.R.; Pradervand, C.; Thominet, V.; Schneider, R.; Panepucci, E.; Grunder, M.; Gabadinho, J.; Dworkowski, F.S.N.; Tomizaki, T.; Schneider, J.; Mayer, A.; Curtin, A.; Olieric, V.; Frommherz, U.; Kotrle, G.; Welte, J.; Wang, X.; Maag, S.; Schulze-Briese, C.; Wang, M.

doi:10.1107/S160057751400006X

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Figure 9
Beam paths of the MS3 microspectrophotometer. All optical axes converge at two beamsplitters underneath the reflective Schwarzschild microscope objective. From there they are deflected on-axis with the X-ray beam by a drilled 45° mirror behind the objective. The imaging branch of the sample-viewing microscope is split by a further beamsplitter into a low-magnification and a high-magnification fixed-zoom branch with separate firewire CCD cameras (Point Grey GRAS-20S4-C). The spectroscopic unit contains the beamsplitter separating the excitation from the detection branch, both coupled via light fibers to various lasers and the spectrographs, respectively.

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

Volume 21| Part 2| February 2014| Pages 340-351

doi:10.1107/S160057751400006X

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