have plotted the coincidence rate as a function of the geometric mean of the signal
and idler count rates; in fact, because the efficiency of the two detectors is
different, we measure different single-photon count rates in the two channels.
Dark counts have been subtracted from the plotted count rates. For the coincidence
rates, both dark–dark and photon–dark coincidences have to be taken in account,
but for the counting rates in our experiment the former are negligible. Thus far,
we have achieved a maximum coincidence rate of 10
3
counts/s (= coincidence
rate/pulse gate-pulse rate), which is expected to go up by at least a factor of
10 with use of a higher repetition-rate gate-pulse generator.
We have performed two independent experiments to demonstrate ...