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Figure 3
Top: experimental and simulated η distributions for a 25 µm-pitch strip sensor, normalized to integrated counts. The simulated peaks are closer to 0 and 1 than in the experimental distribution owing to reduced charge sharing as a result of underestimating the strip coupling in the simulation. Bottom: introduction of the coupling factor K = 0.06 yields agreement within experimental error between experiment and simulation.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 19| Part 3| March 2012| Pages 359-365
doi:10.1107/S090904951200235X
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