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Figure 3
Measured rate response obtained from the standard user fill paralyzable detector with no pulse rejection [equation (2)[link]] with shaping time as a free parameter. The largest shaping time [\tau_{\rm s}] was modelled well while the smallest shaping times were clearly not modelled by the expected non-bunched formula.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
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