Development of novel plastic scintillators based on polyvinyltoluene for the hybrid j-pet/mr tomograph


Table 6 Constitution of plastic scintillators containing new wavelength shifters



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Table 6 Constitution of plastic scintillators containing new wavelength shifters. 
Polymeric base 
Primary additive 
Secondary fluor 
Polystyrene 
p-terphenyl (PTP) /
2,5-diphenyloxazole (PPO) 
1 % 
Synthesized substances in 
amount 
0.01 % 
Scintillators were cut and polished to a geometry of cylinder with diameter and 
height equal to 2.5 cm. They were wrapped with teflon foil and their interaction with 
gamma quanta from 
68
Ge source was tested. A simple experimental setup consisting of 
vacuum photomultiplier, scintillator and source was built (Fig. 6) and charge spectra were 
registered.
P(OEt)
3


28 
Figure 6 Experimental setup for the estimation of plastic scintillators light output. 
Detailed analysis of spectra registered during gamma quanta interaction with plastic 
scintillator and description of the phenomenon itself are the subject of
Chapter 7.2: Spectral properties of J-PET scintillators. The first preliminary studies relied 
on fitting Fermi function to the falling edge of the spectrum. That allows to estimate 
roughly the relative light yield of tested scintillators. Fermi function is given by the 
equation (1): 
(1). 
Parameters denoted as P
0
, P
1
, P
2
, P
3
are related to maximal values of the function, the 
middle of the edge, slope and minimal values of the function, respectively.
The function was fitted to spectra as it is shown in Fig. 7 registered for stilbene 
which was taken as standard. In the spectrum, histogram of signals amplitudes is presented. 
Amplitudes are proportional to the number of photons produced by scintillator during 
interaction with gamma quanta. The absolute number of photons produced by scintillator 
interacting with gamma quanta was not calculated. The aim of this test was to check if 
developed materials have a potential for being used as scintillators. 


29 
P
1
parameter describing the middle of the falling edge, was a measure of 
scintillators light output. P
1
determined for obtained scintillators were compared to the 
parameter value of stilbene. Results of such rough estimation of scintillators light output 
are presented in Tab. 7. 

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