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Figure 4
Dark-current measurements of each ion chamber (a) I0, (b) I1, (c) I2. The dark current can then be subtracted. The discontinuity follows a change in detector gain. (d) This noise is included in the variance in counts in the uncertainty of the EXAFS spectra.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 30| Part 1| January 2023| Pages 147-168
https://doi.org/10.1107/S1600577522010293
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