Radiation detectors have two main detection mechanisms:
direct conversion, which utilises a photoconductor to directly
convert radiation into an electrical signal, and indirect
conversion, which utilises a scintillator to convert radiation into
visible light, which is subsequently converted into an electrical
signal. The photoconductor material, mercury (II) iodide (HgI2)
sensitive to visible light, has the property of gradually decreasing
signal for repeated irradiation beams. Therefore, this study aimed
to improve the signal magnitude and stability to repeated
measurements of polycrystalline HgI2 by mixing 0, 4, 6, 8, 10,
and 20 weight percent (wt%) of terbium-doped gadolinium oxysulfide
(GOS:Tb), a scintillator material that emits visible light. The
performance of these dosimeters was evaluated with a focus on
dosimetric parameters such as signal quantity, short-term
repeatability, dose-response linearity, and dose-rate dependence to
assess their potential application in radiotherapy quality assurance
(QA). The results from the dosimeters were compared with those from
a metal-oxide-semiconductor field-effect transistor (MOSFET)
dosimeter and an ionisation chamber. Peak was found for the
dosimeter with 8 wt% GOS:Tb but decreased for the dosimeters with
10 and 20 wt% GOS:Tb. The standard deviations of short-term
repeatability were 1.45%, 0.86%, 1.18%, 1.51%, 131%, and 4.48%
for dosimeters with 0, 4, 6, 8, 10, and 20 wt% GOS:Tb,
respectively. The dosimeters with 4 and 6 wt% GOS:Tb had better
standard deviations of repeatability than the MOSFET (1.35%), but
not better than the ionization chamber (0.5%). All dosimeters, the
MOSFET, and the ion chamber demonstrated excellent dose-response
linearity for monitor unit (MU) values ranging from 2 to 500, with
R
2 values exceeding 0.9997. The sensitivity analysed using the
linear slope was the highest for the dosimeter with 6 wt% GOS:Tb
(0.103) and the MOSFET (0.0103) among all dosimeters. The dosimeter
with 6 wt% GOS:Tb and the MOSFET exhibited deviations of 4.64%
and 3.31%, respectively, at a dose rate of 100 cGy/min, thus
failing to meet the evaluation standard of within 2%. The ion
chamber, however, achieved compliance with a deviation of 0.15%.
Therefore, it is necessary to apply correction factors to each dose
rate when using hybrid dosimeters for QA. The optimal mixing ratio
of GOS:Tb for manufacturing the hybrid dosimeter was determined to
be 6 wt%, suggesting signal amplification through visible light
and a potential improvement in operational stability through pore
filling of the material.