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 |