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      KCI등재 SCI SCIE SCOPUS

      Dosimetric Accuracy of AAA and Acuros XB Dose Calculations within an Air Cavity for Small Fields of a 6-MV Flattening Filter-free Beam

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      https://www.riss.kr/link?id=A104130758

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      다국어 초록 (Multilingual Abstract)

      The purpose of this research were to verify the accuracy of dose calculation by using the analytical anisotropic algorithm (AAA) and Acuros XB (AXB) against measurements within an air cavity for small fields from a 6-MV flattening filter-free (FFF) beam. A rectangular slab phantom containing an air cavity was specially constructed for this study. Computed tomography (CT) image data sets were acquired with and without a film at four selected depths (4.5, 5.5, 6.5, and 7.5 cm) in the air cavity of the phantom for the dose calculation. The central-axis point dose (CAPD) and dose profile were measured with the film at selected depths for field sizes from 2 × 2 to 5 × 5 cm2 along the central-beam axis of a 6-MV FFF beam. The central-axis doses (CADs) and dose profiles calculated by using both the AAA and AXB were obtained by using an Eclipse treatment planning system (TPS) under the same measurement conditions. The calculation algorithms were denoted as AXB w and AAA w when the film was included in an air cavity of the phantom and an AXB w/o and AAA w/o when no film was included. The accuracy of the CAD and dose profile calculated by using both algorithms were compared with the measured CAPD and dose profile, and their differences were evaluated by using root-mean square-error (RMSE) and gamma-index analyse. The percentage difference (%Diff) of the CAD calculated by using AXB w showed good agreement (within 5%) with the measured CAPD at selected depths in the air cavity. However, the corresponding values for the other algorithms, especially AAA w and AAA w/o appeared to exhibit relatively high disagreement. The maximum %Diffs between the calculated CAD and the measured CAPD were 4.8% and −39.4% for the AXB w and AXB w/o, respectively. The %Diffs increased with decreasing field size and increasing measurement depth. For the calculated and the measured dose profiles, the RMSE values for AXB w were within 9.3 cGy in both the inner profile and the penumbra whereas the RMSE values for AAA w produced a wide range (52.2 − 96.8 cGy). This study demonstrated that the dose calculated by using AXB was more accurate than that calculated by using the AAA when compared to the measured dose in the air cavity. In addition, we observed that AXB w was superior to AXB w/o in this region with respect to the measurements.
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      The purpose of this research were to verify the accuracy of dose calculation by using the analytical anisotropic algorithm (AAA) and Acuros XB (AXB) against measurements within an air cavity for small fields from a 6-MV flattening filter-free (FFF) be...

      The purpose of this research were to verify the accuracy of dose calculation by using the analytical anisotropic algorithm (AAA) and Acuros XB (AXB) against measurements within an air cavity for small fields from a 6-MV flattening filter-free (FFF) beam. A rectangular slab phantom containing an air cavity was specially constructed for this study. Computed tomography (CT) image data sets were acquired with and without a film at four selected depths (4.5, 5.5, 6.5, and 7.5 cm) in the air cavity of the phantom for the dose calculation. The central-axis point dose (CAPD) and dose profile were measured with the film at selected depths for field sizes from 2 × 2 to 5 × 5 cm2 along the central-beam axis of a 6-MV FFF beam. The central-axis doses (CADs) and dose profiles calculated by using both the AAA and AXB were obtained by using an Eclipse treatment planning system (TPS) under the same measurement conditions. The calculation algorithms were denoted as AXB w and AAA w when the film was included in an air cavity of the phantom and an AXB w/o and AAA w/o when no film was included. The accuracy of the CAD and dose profile calculated by using both algorithms were compared with the measured CAPD and dose profile, and their differences were evaluated by using root-mean square-error (RMSE) and gamma-index analyse. The percentage difference (%Diff) of the CAD calculated by using AXB w showed good agreement (within 5%) with the measured CAPD at selected depths in the air cavity. However, the corresponding values for the other algorithms, especially AAA w and AAA w/o appeared to exhibit relatively high disagreement. The maximum %Diffs between the calculated CAD and the measured CAPD were 4.8% and −39.4% for the AXB w and AXB w/o, respectively. The %Diffs increased with decreasing field size and increasing measurement depth. For the calculated and the measured dose profiles, the RMSE values for AXB w were within 9.3 cGy in both the inner profile and the penumbra whereas the RMSE values for AAA w produced a wide range (52.2 − 96.8 cGy). This study demonstrated that the dose calculated by using AXB was more accurate than that calculated by using the AAA when compared to the measured dose in the air cavity. In addition, we observed that AXB w was superior to AXB w/o in this region with respect to the measurements.

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      참고문헌 (Reference)

      1 A. Fogliata, 52 : 1363-, 2007

      2 B. M. Prendergast, 14 : 64-, 2013

      3 L. Tillikainen, 53 : 3821-, 2008

      4 S. Lang, 106 : 255-, 2013

      5 M. W. K. Kan, 39 : 4705-, 2012

      6 K. Bush, 38 : 2208-, 2011

      7 S. Rana, 38 : 9-, 2013

      8 C. -M. Ma, 56 : 3073-, 2011

      9 M. W. L. Kan, 56 : 397-, 2011

      10 S. Devic, 27 : 112-, 2011

      1 A. Fogliata, 52 : 1363-, 2007

      2 B. M. Prendergast, 14 : 64-, 2013

      3 L. Tillikainen, 53 : 3821-, 2008

      4 S. Lang, 106 : 255-, 2013

      5 M. W. K. Kan, 39 : 4705-, 2012

      6 K. Bush, 38 : 2208-, 2011

      7 S. Rana, 38 : 9-, 2013

      8 C. -M. Ma, 56 : 3073-, 2011

      9 M. W. L. Kan, 56 : 397-, 2011

      10 S. Devic, 27 : 112-, 2011

      11 P. R. Almond, 26 : 1847-, 1999

      12 J. M. Moran, 6 : 62-, 2005

      13 J. Y. Park, 38 : 6688-, 2011

      14 T. Han, 38 : 2651-, 2011

      15 A. Fogliata, 6 : 82-, 2011

      16 W. Ulmer, 50 : 1767-, 2005

      17 C. Y. Huang, 57 : 826-, 2002

      18 B. H. Shahine, 26 : 350-, 1999

      19 P. Carrasco, 31 : 2899-, 2004

      20 정현욱, "Photon Beam Dosimetry with EBT3 Film in Heterogeneous Regions: Application to the Evaluation of Dose-calculation Algorithms" 한국물리학회 65 (65): 1829-1838, 2014

      21 정진범, "Comparison of Anisotropic Analytic Algorithm Plan and Acuros XB Plan for Lung Stereotactic Ablative Radiotherapy Using Flattening Filter-Free Beams" 한국의학물리학회 25 (25): 210-217, 2014

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      학술지 이력
      연월일 이력구분 이력상세 등재구분
      2023 평가예정 해외DB학술지평가 신청대상 (해외등재 학술지 평가)
      2020-01-01 평가 등재학술지 유지 (해외등재 학술지 평가) KCI등재
      2011-01-01 평가 등재학술지 유지 (등재유지) KCI등재
      2009-01-01 평가 등재학술지 유지 (등재유지) KCI등재
      2007-01-01 평가 SCI 등재 (등재유지) KCI등재
      2005-01-01 평가 등재학술지 유지 (등재유지) KCI등재
      2002-07-01 평가 등재학술지 선정 (등재후보2차) KCI등재
      2000-01-01 평가 등재후보학술지 선정 (신규평가) KCI등재후보
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      기준연도 WOS-KCI 통합IF(2년) KCIF(2년) KCIF(3년)
      2016 0.47 0.15 0.31
      KCIF(4년) KCIF(5년) 중심성지수(3년) 즉시성지수
      0.26 0.2 0.26 0.03
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