Surface and build‐up dose comparison between Elekta 6 MV flattening filter and flattening‐filter‐free beams using an advanced Markus ionization chamber and a solid water‐equivalent phantom
Using a plane‐parallel advanced Markus ionization chamber and a stack of water‐equivalent solid phantom blocks, percentage surface and build‐up doses of Elekta 6 MV flattening filter (FF) and flattening‐filter‐free (FFF) beams were measured as a function of the phantom depth for field sizes ranging...
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Published in: | Journal of applied clinical medical physics Vol. 21; no. 12; pp. 334 - 339 |
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Abstract | Using a plane‐parallel advanced Markus ionization chamber and a stack of water‐equivalent solid phantom blocks, percentage surface and build‐up doses of Elekta 6 MV flattening filter (FF) and flattening‐filter‐free (FFF) beams were measured as a function of the phantom depth for field sizes ranging from 2 × 2 to 10 × 10 cm2. It was found that the dose difference between the FF and the FFF beams was relatively small. The maximum dose difference between the FF and the FFF beams was 4.4% at a depth of 1 mm for a field size of 2 × 2 cm2. The dose difference was gradually decreased while the field size was increased up to 10 × 10 cm2. The measured data were also compared to published Varian FF and FFF data, suggesting that the percentage surface and build‐up doses as well as the percentage dose difference between FF and FFF beams by our Elekta linac were smaller than those by the Varian linac. |
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AbstractList | Using a plane-parallel advanced Markus ionization chamber and a stack of water-equivalent solid phantom blocks, percentage surface and build-up doses of Elekta 6 MV flattening filter (FF) and flattening-filter-free (FFF) beams were measured as a function of the phantom depth for field sizes ranging from 2 × 2 to 10 × 10 cm
. It was found that the dose difference between the FF and the FFF beams was relatively small. The maximum dose difference between the FF and the FFF beams was 4.4% at a depth of 1 mm for a field size of 2 × 2 cm
. The dose difference was gradually decreased while the field size was increased up to 10 × 10 cm
. The measured data were also compared to published Varian FF and FFF data, suggesting that the percentage surface and build-up doses as well as the percentage dose difference between FF and FFF beams by our Elekta linac were smaller than those by the Varian linac. Using a plane‐parallel advanced Markus ionization chamber and a stack of water‐equivalent solid phantom blocks, percentage surface and build‐up doses of Elekta 6 MV flattening filter (FF) and flattening‐filter‐free (FFF) beams were measured as a function of the phantom depth for field sizes ranging from 2 × 2 to 10 × 10 cm 2 . It was found that the dose difference between the FF and the FFF beams was relatively small. The maximum dose difference between the FF and the FFF beams was 4.4% at a depth of 1 mm for a field size of 2 × 2 cm 2 . The dose difference was gradually decreased while the field size was increased up to 10 × 10 cm 2 . The measured data were also compared to published Varian FF and FFF data, suggesting that the percentage surface and build‐up doses as well as the percentage dose difference between FF and FFF beams by our Elekta linac were smaller than those by the Varian linac. Using a plane‐parallel advanced Markus ionization chamber and a stack of water‐equivalent solid phantom blocks, percentage surface and build‐up doses of Elekta 6 MV flattening filter (FF) and flattening‐filter‐free (FFF) beams were measured as a function of the phantom depth for field sizes ranging from 2 × 2 to 10 × 10 cm2. It was found that the dose difference between the FF and the FFF beams was relatively small. The maximum dose difference between the FF and the FFF beams was 4.4% at a depth of 1 mm for a field size of 2 × 2 cm2. The dose difference was gradually decreased while the field size was increased up to 10 × 10 cm2. The measured data were also compared to published Varian FF and FFF data, suggesting that the percentage surface and build‐up doses as well as the percentage dose difference between FF and FFF beams by our Elekta linac were smaller than those by the Varian linac. Using a plane‐parallel advanced Markus ionization chamber and a stack of water‐equivalent solid phantom blocks, percentage surface and build‐up doses of Elekta 6 MV flattening filter (FF) and flattening‐filter‐free (FFF) beams were measured as a function of the phantom depth for field sizes ranging from 2 × 2 to 10 × 10 cm2. It was found that the dose difference between the FF and the FFF beams was relatively small. The maximum dose difference between the FF and the FFF beams was 4.4% at a depth of 1 mm for a field size of 2 × 2 cm2. The dose difference was gradually decreased while the field size was increased up to 10 × 10 cm2. The measured data were also compared to published Varian FF and FFF data, suggesting that the percentage surface and build‐up doses as well as the percentage dose difference between FF and FFF beams by our Elekta linac were smaller than those by the Varian linac. |
Author | Takenaka, Shigeharu Imae, Toshikazu Aoki, Atsushi Abe, Osamu Nawa, Kanabu Nakagawa, Keiichi Watanabe, Yuichi Matsuda, Kanako Sasaki, Katsutake Saegusa, Shigeki |
AuthorAffiliation | 1 Department of Radiology University of Tokyo Hospital Tokyo Japan 2 Faculty of Health Sciences Komazawa University Tokyo Japan |
AuthorAffiliation_xml | – name: 2 Faculty of Health Sciences Komazawa University Tokyo Japan – name: 1 Department of Radiology University of Tokyo Hospital Tokyo Japan |
Author_xml | – sequence: 1 givenname: Toshikazu orcidid: 0000-0002-6850-3806 surname: Imae fullname: Imae, Toshikazu email: imaet-rad@h.u-tokyo.ac.jp organization: University of Tokyo Hospital – sequence: 2 givenname: Shigeharu surname: Takenaka fullname: Takenaka, Shigeharu organization: University of Tokyo Hospital – sequence: 3 givenname: Yuichi surname: Watanabe fullname: Watanabe, Yuichi organization: Komazawa University – sequence: 4 givenname: Atsushi surname: Aoki fullname: Aoki, Atsushi organization: University of Tokyo Hospital – sequence: 5 givenname: Kanako surname: Matsuda fullname: Matsuda, Kanako organization: University of Tokyo Hospital – sequence: 6 givenname: Katsutake surname: Sasaki fullname: Sasaki, Katsutake organization: University of Tokyo Hospital – sequence: 7 givenname: Shigeki surname: Saegusa fullname: Saegusa, Shigeki organization: University of Tokyo Hospital – sequence: 8 givenname: Kanabu surname: Nawa fullname: Nawa, Kanabu organization: University of Tokyo Hospital – sequence: 9 givenname: Keiichi surname: Nakagawa fullname: Nakagawa, Keiichi organization: University of Tokyo Hospital – sequence: 10 givenname: Osamu surname: Abe fullname: Abe, Osamu organization: University of Tokyo Hospital |
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Cites_doi | 10.1118/1.596896 10.1007/s11604-006-0094-2 10.1118/1.596522 10.1120/jacmp.v16i3.5219 10.1088/0031-9155/50/3/002 10.1088/0031-9155/61/23/8360 10.1016/j.ijrobp.2011.12.064 10.1118/1.3554643 10.1118/1.3190392 10.1088/0031-9155/53/7/009 |
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Keywords | flattening-filter-free (FFF) beam flattening filter (FF) beam a solid water-equivalent phantom surface dose build-up ionization chamber |
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References | 2012; 83 2009; 36 1992; 19 2016; 61 2015; 16 2005; 50 2008; 53 2011; 38 1990; 17 2007; 25 2018; 15 e_1_2_8_3_1 e_1_2_8_2_1 e_1_2_8_5_1 Aoki S (e_1_2_8_4_1) 2018; 15 e_1_2_8_7_1 e_1_2_8_6_1 e_1_2_8_9_1 e_1_2_8_8_1 e_1_2_8_10_1 e_1_2_8_11_1 e_1_2_8_12_1 |
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Snippet | Using a plane‐parallel advanced Markus ionization chamber and a stack of water‐equivalent solid phantom blocks, percentage surface and build‐up doses of Elekta... Using a plane-parallel advanced Markus ionization chamber and a stack of water-equivalent solid phantom blocks, percentage surface and build-up doses of Elekta... |
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SubjectTerms | a solid water‐equivalent phantom build‐up Dosimetry flattening filter (FF) beam flattening‐filter‐free (FFF) beam ionization chamber Polymethyl methacrylate Standard deviation surface dose Technical Note Technical Notes |
Title | Surface and build‐up dose comparison between Elekta 6 MV flattening filter and flattening‐filter‐free beams using an advanced Markus ionization chamber and a solid water‐equivalent phantom |
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