Positron emission tomography–computed tomography (PET–CT) with internal administration of the FDG-18 is characterized as a widespread functional imaging modality in diagnostic radiation medicine, which increases the patient effective doses owing to the presence of internal and external radiation sources. Hence, patient effective dose estimation has been pinpointed as a significant factor in radiation protection assessment. A large number of studies have been published in this regard, and various dosimetry methods have been surveyed. According to our previous research, 10 patients had participated in PET–CT scans with three static time sequences imaging. PET effective doses were estimated using a simple method derived from Anderson et al. and Kaushik et al. coefficients, and the CT effective doses were surveyed with a CTDI phantom and cylindrical ionization chamber. The CT dose was tripled owing to the three static time-sequences imaging. The effective doses were calculated using different coefficients and the results of the PET effective doses were compared. The PET–CT effective dose was varied from 17.14 to 18.42 mSv based on Kaushik et al. coefficients which were measured for one low-dose CT scan. This study aimed to survey simple PET–CT effective dose estimation using three static-time imaging approaches which increases the total patient effective doses.
Purpose:
Accurate dosimetery is very essential in diagnostic radiology. The goal of this study is to verify the application of LiF:Mg,Cu,P (TLD100H) in obtaining the Entrance skin dose (ESD) of patients undergoing diagnostic radiology. The results of dosimetry performed by TLD‐100H, were compared with those obtained by TLD100, which is a common dosimeter in diagnostic radiology.
Methods:
In this study the ESD values were measured using two types of Thermoluminescence dosimeters (TLD‐100, and TLD‐100H) for 16 patients undergoing diagnostic radiology (lumbar spine imaging). The ESD values were also obtained by putting the two types of TLDs at the surface of Rando phantom for different imaging techniques and different views (AP, and lateral). The TLD chips were annealed with a standard procedure, and the ECC values for each TLD was obtained by exposing the chips to equal amount of radiation. Each time three TLD chips were covered by thin dark plastic covers, and were put at the surface of the phantom or the patient. The average reading of the three chips was used for obtaining the dose.
Results:
The results show a close agreement between the dose measuered by the two dosimeters.According to the results of this study, the TLD‐100H dosimeters have higher sensitivities (i.e.signal(nc)/dose) than TLD‐100. The ESD values varied between 2.71 mGy and 26.29 mGy with the average of 11.89 mGy for TLD‐100, and between 2.55 mGy and 27.41 mGy with the average of 12.32 mGy for measurements.
Conclusion:
The TLD‐100H dosimeters are suggested as effective dosimeters for dosimetry in low dose fields because of their higher sensitivities.
Estimating internal contamination from 131I for children in nuclear accidents is a crucial subject in the radiation protection field. Throughout this paper, an urgent and simple method was proposed for measuring 131I inside the pediatric thyroid gland by constructing a neck and thyroid phantom. For this purpose, CT scan images of healthy child’s thyroids were obtained, and the sizes of different parts were determined by a 3D slicer image processing software. Girls with the body surface area between 0.95 and 1.05 were involved in this study. The fabricated phantom is composed of 5 cylindrical slabs of 2-cm thickness, and several small holes were constructed for TLD dosemeters near the thyroid gland and all other parts of the neck. The phantom was constructed utilizing a 3D printer with acrylonitrile butadiene styrene plastic. The thyroid phantom was filled with radioiodine-131, and calibration curves were plotted for contamination estimation. A nodular thyroid phantom was also constructed. The nodular phantom or the resolution phantom has 4 removable parts containing cylindrical holes with diameters of 3, 6, 9 and 12 mm. These holes on the thyroid glands can be filled with different activities of radionuclides to serve as hot and cold spots for quality control of nuclear medicine images. The results show that the designed phantom is applicable in different fields such as nuclear image quality and resolution tests, dosimetry and iodine thyroid uptake estimation in nuclear medicine departments, and nuclear emergency monitoring.
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