TABLE I.
Variables and parameters used within the theoretical model of coaxial prompt γ-ray detection, cf. fig. 1.
z | beam axis coordinate | [mm] |
z0 | front face position of water target | 0 mm |
zd | front face position of the detector | 152 mm |
L | length of the water phantom | 150 mm |
Rw | proton range in water | [mm] |
r | detector radius | ½” |
t | detector thickness | 1½” |
Nγ | γ-rays emitted per incident proton | [ ] |
prompt γ-ray yield per unit length | 6·10−4 mm−1 | |
distal falloff slope | 0.3 mm−1 | |
transmission probability | [ ] | |
average absorption coefficient of water | 10−4 mm−1 | |
relative solid angle subtended | [ ] | |
probability of interaction in detector | [ ] | |
average attenuation coefficient of detector | 2·10−2 mm−1 | |
td | decay time of the scintillation light pulse | 16 ns |
Np | number of protons within one spot cluster | 108 |
prompt γ-rays detected per proton (theory) | [ ] | |
Nd | prompt γ-rays detected per spot (theory | [ ] |
Md | prompt γ-rays measured per spot cluster | [ ] |
ratio between all counts and the prompt γ-rays | 2.5 | |
overall detector count rate | [Mcps] | |
Ip | the proton beam (peak) current at the target | 2 nA |
e | elementary charge | 1.6·10−19 C |
absolute error in the proton range Rw | 1 mm | |
absolute error in the phantom position z0 | 1 mm | |
κ | thickness of a cavity within the water target | 2 mm |
zκ | front face position of a cavity within the target | [mm] |
ΔN | relative count variation for a range error δR | [ ] |
relative count variation for a target error δz | [ ] | |
γ-ray emission variation for a range error δR | [ ] | |
relative count variation due to a cavity κ | [ ] | |
Δs | statistical measurement uncertainty | [ ] |
background fraction separated by energy filters | 0.5 | |
proton bunch time spread (FWHM) | 2 ns | |
Tp | proton bunch period | 9.4 ns |