
4 Principle of Data Acquisition
Three of the CFD channels are used for the detector signals. The CFD output pulses of these
channels are fed directly into the ECL inputs of the TDC chip. The fourth CFD input is used
for the reference from the laser. Before the reference pulses enter the TDC chip they pass a
frequency divider, FD, and a synchronisation circuit, SYNC. The divider ratio of FD is select-
able and can be set to 1:1, 1:2, or 1:4. The subsequent synchronisation circuit transmits one -
and only one - synchronisation pulse if one of the first three CFDs has received a photon pulse
within the previous pulse period of the divided reference signal. Thus, TDC2 receives one
reference pulse when at least one photon was recorded in the previous 1, 2, or 4 excitation
periods. As a result, the reference pulse rate is reduced to less than the photon rate. The reduc-
tion is achieved without sacrificing any excitation periods or photons.
Pulse diagrams for FD = 1:1 and FD = 2:1 are shown in Fig. 5 and Fig. 6, respectively. With
FD = 1:1 the time of a photon is measured with respect to the next reference pulse. Thus, the
measurement time interval extends over one period of the light source.
With FD = 2:1 (Fig. 6) the photon time is measured with respect to the next or second next
excitation pulse, depending on whether the photon was detected in an even or uneven excita-
tion period. Thus, the measurement time interval extends over 2 laser periods. A frequency
divider ratio of four results in a recording over four signal periods.
Reference,
from laser
Photons
reference
Time of photon
Time of photon
Recorded
pulse
Interval
recorded
Fig. 5: Reference synchronisation for FD=1:1. After the detection of a photon the next reference pulse is re-
corded. The time of the photon is measured with respect to the selected pulse.
Reference,
from laser
Photons
Reference
after
SYNC
Time of photon
Time of photon
Reference,
after FD=2
Interval
recorded
Fig. 6: Reference synchronisation for FD=2:1. The reference pulses are divided by a ratio of 2:1. After the detec-
tion of a photon the next pulse from the frequency divider is recorded. The time of the photon is measured with
respect to this pulse. The measurement time interval extends over 2 reference periods.
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