2002
DOI: 10.1118/1.1508108
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An investigation of a new amorphous silicon electronic portal imaging device for transit dosimetry

Abstract: The relationship between the pixel value and exit dose was investigated for a new commercially available amorphous silicon electronic portal imaging device. The pixel to dose mapping function was established to be linear for detector distances between 116.5 cm to 150 cm from the source, radiation field sizes from 5 x 5 cm2 to 20 x 20 cm2 and beam energies of 6 to 18 MV. Coefficients in the mapping function were found to be dependent on beam energy and field size. Open and wedged field profiles measured with th… Show more

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Cited by 77 publications
(63 citation statements)
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“…Their response characteristics with respect to various input parameters have been investigated by sev-eral groups, [4][5][6][7][8][9][10][11] which suggest the appropriateness of using this type of EPID for dose measurement. Throughout this paper, EPID refers to the amorphous silicon-based EPID unless otherwise stated.…”
Section: Introductionmentioning
confidence: 99%
“…Their response characteristics with respect to various input parameters have been investigated by sev-eral groups, [4][5][6][7][8][9][10][11] which suggest the appropriateness of using this type of EPID for dose measurement. Throughout this paper, EPID refers to the amorphous silicon-based EPID unless otherwise stated.…”
Section: Introductionmentioning
confidence: 99%
“…Although it is implemented in several different departments as the routine method for IMRT pre-treatment verification [20][21][22][23][24][25][26][27], little information is available in the literature on the criteria to use for the analysis and acceptance/rejection of the acquired data. In addition, the commercially available solution suffers from a suboptimal calibration procedure that limits the achievable accuracy for larger field sizes or highly asymmetrical fields.…”
mentioning
confidence: 99%
“…Different QA measurement techniques in IMRT exist, making use of 2D detector array [5][6][7][8], single ion chamber in phantom for point dose measurements [9][10][11] or using specific phantoms with 2D dose measurement devices and 3D dose reconstruction software [12][13][14]. One disadvantage of these approaches is that measurements are generally compared with calculations by the TPS and it is difficult to give interpretation and to address the deviations between calculated and measured doses to failures of the accelerator performance or to the calculation algorithm.…”
Section: Introductionmentioning
confidence: 99%