Concepts for dose determination in flat-detector CT
Autor: | Oliver Langner, Paul Deak, Willi A. Kalender, Yiannis Kyriakou |
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Rok vydání: | 2008 |
Předmět: |
Physics
Radiological and Ultrasound Technology Phantoms Imaging business.industry Computed tomography dose index Monte Carlo method Reproducibility of Results Radiation Dosage Imaging phantom Pencil (optics) Kerma Optics Ionization Calibration Dosimetry Computer Simulation Radiology Nuclear Medicine and imaging Thermoluminescent dosimeter Radiometry Tomography X-Ray Computed business Nuclear medicine Head Monte Carlo Method Whole-Body Irradiation |
Zdroj: | Physics in Medicine and Biology. 53:3551-3566 |
ISSN: | 1361-6560 0031-9155 |
Popis: | Flat-detector computed tomography (FD-CT) scanners provide large irradiation fields of typically 200 mm in the cranio-caudal direction. In consequence, dose assessment according to the current definition of the computed tomography dose index CTDI(L=100 mm), where L is the integration length, would demand larger ionization chambers and phantoms which do not appear practical. We investigated the usefulness of the CTDI concept and practical dosimetry approaches for FD-CT by measurements and Monte Carlo (MC) simulations. An MC simulation tool (ImpactMC, VAMP GmbH, Erlangen, Germany) was used to assess the dose characteristics and was calibrated with measurements of air kerma. For validation purposes measurements were performed on an Axiom Artis C-arm system (Siemens Medical Solutions, Forchheim, Germany) equipped with a flat detector of 40 cm x 30 cm. The dose was assessed for 70 kV and 125 kV in cylindrical PMMA phantoms of 160 mm and 320 mm diameter with a varying phantom length from 150 to 900 mm. MC simulation results were compared to the values obtained with a calibrated ionization chambers of 100 mm and 250 mm length and to thermoluminesence (TLD) dose profiles. The MCs simulations were used to calculate the efficiency of the CTDI(L) determination with respect to the desired CTDI(infinity). Both the MC simulation results and the dose distributions obtained by MC simulation were in very good agreement with the CTDI measurements and with the reference TLD profiles, respectively, to within 5%. Standard CTDI phantoms which have a z-extent of 150 mm underestimate the dose at the center by up to 55%, whereas a z-extent of 600 mm appears to be sufficient for FD-CT; the baseline value of the respective profile was within 1% to the reference baseline. As expected, the measurements with ionization chambers of 100 mm and 250 mm offer a limited accuracy, whereas an increased integration length of 600 mm appeared to be necessary to approximate CTDI(infinity) in within 1%. MC simulations appear to offer a practical and accurate way of assessing conversion factors for arbitrary dosimetry setups using a standard pencil chamber to provide estimates of CTDI(infinity). This would eliminate the need for extra-long phantoms and ionization chambers or excessive amounts of TLDs. |
Databáze: | OpenAIRE |
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