General ion recombination effect in a liquid ionization chamber in high-dose-rate pulsed photon and electron beams
Creators
- 1. National Institute of Radiological Sciences, National Institutes for Quantum and Radiological Science and Technology, 4-9-1 Anagawa, Inage, Chiba, Chiba 263-8555 (Japan)
- 2. Proton Medical Research Center, University of Tsukuba Hospital, 2 Chome-1-1 Amakubo, Tsukuba, Ibaraki Prefecture 305-8576 (Japan)
- 3. Faculty of Medicine, University of Tsukuba, 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8575 (Japan)
- 4. Department of Radiation Oncology, The Cancer Institute Hospital of Japanese Foundation for Cancer Research, 3 Chome-8-31 Ariake, Koto, Tokyo 135-0063 (Japan)
- 5. Department of Radiology, University of Tsukuba Hospital, 2 Chome-1-1 Amakubo, Tsukuba, Ibaraki Prefecture 305-8576 (Japan)
Description
Liquid ionization chambers (LICs) are highly sensitive to dose irradiation and have small perturbations because of their liquid-filled sensitive volume. They require a sensitive volume much smaller than conventional air-filled chambers. However, it has been reported that the collection efficiency has dependencies on the dose per pulse and the pulse repetition frequency of a pulsed beam. The purpose of this study was to evaluate in detail the dependency of the ion collection efficiency on the pulse repetition frequency. A microLion (PTW, Freiburg, Germany) LIC was exposed to photon and electron beams from a TrueBeam (Varian Medical Systems, Palo Alto, USA) linear accelerator. The pulse repetition frequency was varied, but the dose per pulse was fixed. A theoretical evaluation of the collection efficiency was performed based on Boag's theory. Linear correlations were observed between the frequency and the relative collection for all energies of the photon and electron beams. The decrease in the collected charge was within 1% for all the flattened photon and electron beams, and they were 1.1 and 1.8% for the 6 and 10 MV flattening filter-free photon beams, respectively. The theoretical ion collection efficiency was 0.990 for a 10 MV flattened photon beam with a dose rate of 3 Gy·min−1. It is suggested that the collected charge decreased because of the short time intervals of the beam pulse compared with the ion collection time. Thus, it is important to correctly choose the pulse repetition frequency, particularly when flattening filter-free mode is used for absolute dose measurements.
Availability note (English)
Available from http://dx.doi.org/10.1093/jrr/rrx088; Available from http://www.ncbi.nlm.nih.gov/pmc/articles/PMC5967456Additional details
Identifiers
- DOI
- 10.1093/jrr/rrx088;
Publishing Information
- Journal Title
- Journal of Radiation Research
- Journal Volume
- 59
- Journal Issue
- 3
- Journal Page Range
- p. 282-285
- ISSN
- 0449-3060
INIS
- Country of Publication
- Japan
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 49082992
- Subject category
- S63: RADIATION, THERMAL, AND OTHER ENVIRONMENTAL POLLUTANT EFFECTS ON LIVING ORGANISMS AND BIOLOGICAL MATERIALS;
- Descriptors DEI
- ELECTRON BEAMS; GY RANGE 01-10; ION DOSIMETRY; LIQUID IONIZATION CHAMBERS; PHOTON BEAMS; RADIATION DOSES; RECOMBINATION
- Descriptors DEC
- ABSORBED DOSE RANGE; BEAMS; DOSES; DOSIMETRY; GY RANGE; IONIZATION CHAMBERS; LEPTON BEAMS; MEASURING INSTRUMENTS; PARTICLE BEAMS; RADIATION DETECTORS; RADIATION DOSE RANGES
Optional Information
- Copyright
- Copyright (c) The Author(s) 2018. Published by Oxford University Press on behalf of The Japan Radiation Research Society and Japanese Society for Radiation Oncology.
- Notes
- PMCID: PMC5967456; PMID: 29373670; PUBLISHER-ID: rrx088; OAI: oai:pubmedcentral.nih.gov:5967456