Multifunctional bending magnet beamline with a capillary optic for X-ray fluorescence studies of metals in tissue sections

Roter, B.; Crawford, A.M.; Jin, Q.; Glowacki, A.T.; Lai, B.; Marin, F.S.; Maxey, E.; Shi, X.; Culotta, V.C.; Wildeman, A.S.; Patel, N.K.; O'Halloran, T.V.; Jacobsen, C.

doi:10.1107/S1600577526000925

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Figure 3
Diagram of how a planar sample and its scanning stage are typically mounted at an angle θ relative to normal incidence for scanning X-ray fluorescence microscopy. This means that the beam width W_beam as seen by a sample at normal incidence is broadened to $[W_{{\rm beam}}^{\,\prime}]$ = $[W_{{\rm beam}}\,/\cos\theta]$ [equation (2)

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

Volume 33| Part 2| March 2026| Pages 319-330

https://doi.org/10.1107/S1600577526000925

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