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Suren Kandasamy Dissertation.pdf - University of Surrey

Suren Kandasamy Dissertation.pdf - University of Surrey

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Total number <strong>of</strong> net countsM.Sc <strong>Dissertation</strong>Figure 4.1 shows the graph <strong>of</strong> total number <strong>of</strong> net counts versus supply voltage.This graph was plotted using the values shown in Table 4.1 for LaCl 3 :Ce(10%)detector.29000024000019000014000090000850 900 950 1000 1050 1100 1150 1200 1250Supply voltage(V)Figure 4.1 The counting curve <strong>of</strong> LaCl 3 :Ce(10%) detector as a function <strong>of</strong>supply voltage.The operating voltage was chosen by the high voltage corresponding to the centrepoints on the plateaus [6]. According to the Fig. 4.1 for the LaCl 3 :Ce(10%) detector theoperating voltage has been found as 950 Volts. When using PMTs for scintillatordetectors, there is a trade between dynamic range, linearity (proportionality <strong>of</strong> response)and resolution. This can discussed as follows. The very high photon yields <strong>of</strong> thescintillator could with its fast emission time means that standard PMTs can easilysaturate when operated at nominal anode to cathode biases <strong>of</strong> ~ 1000 V purely due totheir very high gains [10]. This can result in gross non linearities being into spectra.Reducing the PMT bias may reduce these non linearities and extend the dynamic range,but at the expense <strong>of</strong> a deteriorated energy resolution. Therefore, a trade is requiredbetween range, linearity and resolution [10].From the Fig. 4.1 shows below 860 Volts less number <strong>of</strong> counts was recorded.From that point the recorded count was suddenly increased. That means the PMTworking active voltage bias region. The maximum recommended high voltage powerK. <strong>Suren</strong> 18

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