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. 2023 Nov 3;23(21):8951. doi: 10.3390/s23218951

Table 1.

The detection efficiency of TLCC for a point-like source at the center of FOV under the conditions of the simulation and experiment.

Settings of Gamma Emission
Conditions
Nuclide Representative
Energy (keV)
Measured Counts of
Incident Gamma-rays
Counts of
Effective
2-Events
Proportion of Effective Events (%)
Simulation
(N gammas emit within Ω = 0.031 sr at d = 1 m, N is equal to the sum of the emission probability of each energy branch multiplied by the number 107)
N = 13,418,000 133Ba 356 760,871 11,266 1.48
N = 8,499,000 137Cs 661.7 317,619 10,029 3.16
N = 19,983,260 60Co 1173.2/1332.5 585,709 13,415 2.29
Experiment
(Point-like source with radioactivity A, distance d, and acquisition time t)
A = 0.262 MBq
d = 0.25 m
t = 3600 s
133Ba 356 376,788 8253 2.19
A = 1.88 MBq
d = 1 m
t = 1800 s
137Cs 661.7 628,321 13,186 2.10
A = 1.92 MBq
d = 1 m
t = 1800 s
60Co 1173.2/1332.5 1,129,416 20,176 1.79