CA2531467A1 - Method and device for calculating the radiation dose distribution for a radiation treatment system for the purpose of radiation therapy of an animal body - Google Patents
Method and device for calculating the radiation dose distribution for a radiation treatment system for the purpose of radiation therapy of an animal body Download PDFInfo
- Publication number
- CA2531467A1 CA2531467A1 CA002531467A CA2531467A CA2531467A1 CA 2531467 A1 CA2531467 A1 CA 2531467A1 CA 002531467 A CA002531467 A CA 002531467A CA 2531467 A CA2531467 A CA 2531467A CA 2531467 A1 CA2531467 A1 CA 2531467A1
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- CA
- Canada
- Prior art keywords
- cndot
- radiation
- dose
- quality index
- calculating
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- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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Classifications
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- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61N—ELECTROTHERAPY; MAGNETOTHERAPY; RADIATION THERAPY; ULTRASOUND THERAPY
- A61N5/00—Radiation therapy
- A61N5/10—X-ray therapy; Gamma-ray therapy; Particle-irradiation therapy
- A61N5/103—Treatment planning systems
- A61N5/1031—Treatment planning systems using a specific method of dose optimization
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/29—Measurement performed on radiation beams, e.g. position or section of the beam; Measurement of spatial distribution of radiation
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61N—ELECTROTHERAPY; MAGNETOTHERAPY; RADIATION THERAPY; ULTRASOUND THERAPY
- A61N5/00—Radiation therapy
- A61N5/10—X-ray therapy; Gamma-ray therapy; Particle-irradiation therapy
- A61N5/103—Treatment planning systems
- A61N5/1031—Treatment planning systems using a specific method of dose optimization
- A61N2005/1034—Monte Carlo type methods; particle tracking
Abstract
The invention relates to a method for calculating the radiation dose distribution for a radiation treatment system for the purpose of radiation therapy of an animal body, wherein said radiation beam of the radiation treatment system exhibits a specific beam field size and shape at different depths as well as to a device for calculating the radiation dose distribution for a radiation treatment system for the purpose of radiation therapy of an animal body, wherein said radiation beam of the radiation treatment system exhibits a specific beam field size and shape at different depths.
It is an object of the invention to provide a method and device according to the above allowing the calculation of a radiation dose distribution for a radiation treatment system using a limited amount of data whilst preserving the required accuracy.
According to the invention the method is characterized by the steps of i) determining at least one beam quality index being representative for said radiation beam being used, and ii) calculating said radiation dose distribution in said specific beam field using parameterized dose deposition kernels based on said at least one beam quality index.
It is an object of the invention to provide a method and device according to the above allowing the calculation of a radiation dose distribution for a radiation treatment system using a limited amount of data whilst preserving the required accuracy.
According to the invention the method is characterized by the steps of i) determining at least one beam quality index being representative for said radiation beam being used, and ii) calculating said radiation dose distribution in said specific beam field using parameterized dose deposition kernels based on said at least one beam quality index.
Claims (12)
1. Method for calculating the radiation dose distribution for a radiation treatment system for the purpose of radiation therapy of an animal body, wherein said radiation beam of the radiation treatment system exhibits a specific beam field size and shape at different depths, wherein the method is characterized by the steps of:
i) determining at least one beam quality index being representative for said radiation beam being used, and ii) calculating said radiation dose distribution in said specific beam field using parameterized dose deposition kernels based on said at least one beam quality index.
i) determining at least one beam quality index being representative for said radiation beam being used, and ii) calculating said radiation dose distribution in said specific beam field using parameterized dose deposition kernels based on said at least one beam quality index.
2. Method according to claim 1, further characterized by the steps of iii) using for different devices pre-collected measured radiation beam data, said measured radiation beam data comprising:
a) measured phantom dose data at different depths, for different field shapes and sizes and at different energies;
b) calculated dose deposition kernel parameters;
c) measured head scatter factors and output factors that can be transformed into phantom scatter factors for the corresponding field sizes, iv) determining said at least one beam quality index according to step i) using the pre-collected measured radiation beam data according to step iii);
v) associating the dose deposition kernel parameters to said one or a few beam quality index being determined.
a) measured phantom dose data at different depths, for different field shapes and sizes and at different energies;
b) calculated dose deposition kernel parameters;
c) measured head scatter factors and output factors that can be transformed into phantom scatter factors for the corresponding field sizes, iv) determining said at least one beam quality index according to step i) using the pre-collected measured radiation beam data according to step iii);
v) associating the dose deposition kernel parameters to said one or a few beam quality index being determined.
3. Method according to claim 1, further characterized by step vi) using Monte Carlo simulations to simulate said measured data according to step iii).
4. Method according to any one of the preceding claims, further characterized in that said at least one beam quality index is determined by the ratio between the tissue phantom ratio (TPR) measured at d1=20 cm and d2=10 cm depth (TPR20,10).
5. Method according to any one of the preceding claims, further characterized in that said at least one beam quality index is determined by the percentage depth dose (PDD) at d3=10 cm (PDD10).
6. Method according to any one of the claims 2-5, further characterized in that the dose deposition kernels are pencil dose deposition kernels.
7. Method according to any one of the claims 2-5, further characterized in that the dose deposition kernels are point dose deposition kernels.
8. Method according to any one of the preceding claims, characterized in that the dose per energy fluence at the central axis of the radiation beam is determined as:
wherein the parameters are defined as:
and .alpha. = .alpha.1 + .alpha.2z (7e) and where
wherein the parameters are defined as:
and .alpha. = .alpha.1 + .alpha.2z (7e) and where
9. Method according to claim 8, characterized in that the parameters are expressed through µ, which is a function of TPR(d2,d1) (TPR20,10) with the following expressions:
µ = -0.363009.cndot.TPR20,10 3 + 0.709250.cndot.TPR20,10 2 -0.259794.cndot.TPR20,10 - 0.090314 A1 = -0.0042.cndot.µ3 - 0.46571.cndot.µ2 - 0.099992.cndot.µ +
0.0002918 A2 = -1605.6.cndot.µ2 - 64.40.cndot.µ - 1.239 A3 = -0.016.cndot.µ4 - 0.0055.cndot.µ3 - 0.01246.cndot.µ2 +
0.991726.cndot.µ + 0.0002103 A4 = 0.007.cndot.µ3 - 0.1081.cndot.µ2 - 0.01211.cndot.µ - 0.000208 A5 = 0.003.cndot.µ2 + 0.805.cndot.µ + 0.23061 a1 = -2852.cndot.µ3 + 1641.cndot.µ2 + 47.00.cndot.µ + 2.007 a2 = -0.010.cndot.µ - 0.016 B1 = -69680.47.cndot.µ4 - 12517.918.cndot.µ3 - 780.2216.cndot.µ2 -20.948788.cndot.µ - 0.20531052 B2 = -16.675.cndot.µ2 - 2.0546.cndot.µ - 0.06840 B3 = 1.0011.cndot.µ + 8.1.cndot.10 -5 B4 = 0.0033.cndot.µ3 - 0.11080.cndot.µ2 - 0.012183.cndot.µ -0,0002067 B5 = 2290.cndot.µ2 + 225.17.cndot.µ + 7.084 b1 = 5415900.cndot.µ5 +1573050.cndot.µ4 + 180100,6.cndot.µ3 +
10207,44.cndot.µ2 + 285,8012.cndot.µ+3,35788 b2 = -267,83.cndot.µ2 - 26.215.cndot.µ - 0.93285 b3 = 462400.cndot.µ5 + 87700.cndot.µ4 + 5070.5.cndot.µ3 +
9.641.cndot.µ2 - 6.3843.cndot.µ - 0,15488 b4 = -12319.cndot.µ5 - 2953.1.cndot.µ4 - 263.64.cndot.µ3 -
µ = -0.363009.cndot.TPR20,10 3 + 0.709250.cndot.TPR20,10 2 -0.259794.cndot.TPR20,10 - 0.090314 A1 = -0.0042.cndot.µ3 - 0.46571.cndot.µ2 - 0.099992.cndot.µ +
0.0002918 A2 = -1605.6.cndot.µ2 - 64.40.cndot.µ - 1.239 A3 = -0.016.cndot.µ4 - 0.0055.cndot.µ3 - 0.01246.cndot.µ2 +
0.991726.cndot.µ + 0.0002103 A4 = 0.007.cndot.µ3 - 0.1081.cndot.µ2 - 0.01211.cndot.µ - 0.000208 A5 = 0.003.cndot.µ2 + 0.805.cndot.µ + 0.23061 a1 = -2852.cndot.µ3 + 1641.cndot.µ2 + 47.00.cndot.µ + 2.007 a2 = -0.010.cndot.µ - 0.016 B1 = -69680.47.cndot.µ4 - 12517.918.cndot.µ3 - 780.2216.cndot.µ2 -20.948788.cndot.µ - 0.20531052 B2 = -16.675.cndot.µ2 - 2.0546.cndot.µ - 0.06840 B3 = 1.0011.cndot.µ + 8.1.cndot.10 -5 B4 = 0.0033.cndot.µ3 - 0.11080.cndot.µ2 - 0.012183.cndot.µ -0,0002067 B5 = 2290.cndot.µ2 + 225.17.cndot.µ + 7.084 b1 = 5415900.cndot.µ5 +1573050.cndot.µ4 + 180100,6.cndot.µ3 +
10207,44.cndot.µ2 + 285,8012.cndot.µ+3,35788 b2 = -267,83.cndot.µ2 - 26.215.cndot.µ - 0.93285 b3 = 462400.cndot.µ5 + 87700.cndot.µ4 + 5070.5.cndot.µ3 +
9.641.cndot.µ2 - 6.3843.cndot.µ - 0,15488 b4 = -12319.cndot.µ5 - 2953.1.cndot.µ4 - 263.64.cndot.µ3 -
10.2445.cndot.µ - 0.158854.cndot.µ - 0.0003494 and b5 = 14.15.cndot.µ + 1.17168.
10. Device for calculating the radiation dose distribution for a radiation treatment system for the purpose of radiation therapy of an animal body, wherein said radiation beam of the radiation treatment system exhibits a specific beam field size and shape at different depths, characterized in that the device further comprising inputting means arranged for inputting at least one beam quality index being representative for said radiation beam being used to calculating means, said calculating means being arranged for calculating said radiation dose distribution using parameterized dose deposition kernels being based on said at least one beam quality index.
10. Device for calculating the radiation dose distribution for a radiation treatment system for the purpose of radiation therapy of an animal body, wherein said radiation beam of the radiation treatment system exhibits a specific beam field size and shape at different depths, characterized in that the device further comprising inputting means arranged for inputting at least one beam quality index being representative for said radiation beam being used to calculating means, said calculating means being arranged for calculating said radiation dose distribution using parameterized dose deposition kernels being based on said at least one beam quality index.
11. Device according to claim 10, characterized in that the device is a monitor unit (MU) checking device.
12. Device according to claim 10, characterized in that the device is a IMRT treatment MU checking device.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP04078493A EP1674129B1 (en) | 2004-12-23 | 2004-12-23 | Method and device for calculating the radiation dose distribution for a radiation treatment system for the purpose of radiation therapy of an animal body |
EP04078493.6 | 2004-12-23 |
Publications (1)
Publication Number | Publication Date |
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CA2531467A1 true CA2531467A1 (en) | 2006-06-23 |
Family
ID=34928770
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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CA002531467A Abandoned CA2531467A1 (en) | 2004-12-23 | 2005-12-22 | Method and device for calculating the radiation dose distribution for a radiation treatment system for the purpose of radiation therapy of an animal body |
Country Status (11)
Country | Link |
---|---|
US (1) | US7542545B2 (en) |
EP (1) | EP1674129B1 (en) |
JP (1) | JP4936723B2 (en) |
AT (1) | ATE441460T1 (en) |
AU (1) | AU2005239691A1 (en) |
CA (1) | CA2531467A1 (en) |
DE (1) | DE602004022964D1 (en) |
DK (1) | DK1674129T3 (en) |
ES (1) | ES2330936T3 (en) |
PL (1) | PL1674129T3 (en) |
PT (1) | PT1674129E (en) |
Families Citing this family (24)
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US20080123813A1 (en) * | 2006-04-07 | 2008-05-29 | Maurer Calvin R | Automatic selection of multiple collimators |
SE530825C2 (en) * | 2006-05-04 | 2008-09-23 | Scanditronix Wellhoefer Ab | Method and apparatus for determining a correction factor for a radiation dosimeter by integrating contributions from calculated fluence spectra |
US7620147B2 (en) | 2006-12-13 | 2009-11-17 | Oraya Therapeutics, Inc. | Orthovoltage radiotherapy |
US7496174B2 (en) | 2006-10-16 | 2009-02-24 | Oraya Therapeutics, Inc. | Portable orthovoltage radiotherapy |
US8920406B2 (en) | 2008-01-11 | 2014-12-30 | Oraya Therapeutics, Inc. | Device and assembly for positioning and stabilizing an eye |
US8363783B2 (en) | 2007-06-04 | 2013-01-29 | Oraya Therapeutics, Inc. | Method and device for ocular alignment and coupling of ocular structures |
US7801271B2 (en) | 2007-12-23 | 2010-09-21 | Oraya Therapeutics, Inc. | Methods and devices for orthovoltage ocular radiotherapy and treatment planning |
US7792249B2 (en) | 2007-12-23 | 2010-09-07 | Oraya Therapeutics, Inc. | Methods and devices for detecting, controlling, and predicting radiation delivery |
CA2718408A1 (en) * | 2008-03-12 | 2009-09-17 | Sun Nuclear Corp. | Radiation therapy plan dose perturbation system and method |
EP2457237B1 (en) * | 2009-07-23 | 2019-12-11 | Sun Nuclear Corp. | Multiple axes scanning system for measuring radiation from a radiation source |
EP3460529A1 (en) | 2012-05-29 | 2019-03-27 | Sun Nuclear Corporation | Method and system for calorimetry probe |
KR101513130B1 (en) | 2013-09-23 | 2015-04-17 | 부산대학교 산학협력단 | kernel inducing process of X-ray detector |
JP6692115B2 (en) * | 2014-02-25 | 2020-05-13 | 株式会社日立製作所 | Beam position monitoring device and charged particle beam irradiation system |
US10099067B2 (en) | 2014-12-19 | 2018-10-16 | Sun Nuclear Corporation | Radiation therapy dose calculation |
US10617891B2 (en) | 2015-04-23 | 2020-04-14 | Sun Nuclear Corporation | Radiation detector calibration |
JP6588980B2 (en) | 2015-07-01 | 2019-10-09 | 株式会社日立製作所 | Dose distribution calculation device, particle beam therapy device, and dose distribution calculation method |
US11364392B2 (en) * | 2016-02-18 | 2022-06-21 | Convergent R.N.R Ltd. | Method of evaluating a dose as function of depth for nonuniform X-ray beams |
WO2018023049A1 (en) | 2016-07-28 | 2018-02-01 | Sun Nuclear Corporation | Beam angle direction determination |
US10918888B2 (en) | 2017-02-28 | 2021-02-16 | Sun Nuclear Corporation | Radiation therapy treatment verification with electronic portal imaging device transit images |
US11278744B2 (en) | 2018-09-28 | 2022-03-22 | Sun Nuclear Corporation | Systems and methods to account for tilt of a radiation measurement system |
US11600004B2 (en) | 2019-07-10 | 2023-03-07 | Sun Nuclear Corporation | Image-based radiation therapy quality assurance |
WO2021007459A1 (en) | 2019-07-10 | 2021-01-14 | Sun Nuclear Corporation | Scintillator-based radiation therapy quality assurance |
CN110554423B (en) * | 2019-09-30 | 2021-01-01 | 中北大学 | Radiation dose calculation system |
CN115910418A (en) * | 2021-08-05 | 2023-04-04 | 合肥锐视医疗科技有限公司 | Preparation method of radiation protection box body based on Monte Carlo simulation |
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-
2004
- 2004-12-23 DK DK04078493T patent/DK1674129T3/en active
- 2004-12-23 PL PL04078493T patent/PL1674129T3/en unknown
- 2004-12-23 DE DE602004022964T patent/DE602004022964D1/en active Active
- 2004-12-23 PT PT04078493T patent/PT1674129E/en unknown
- 2004-12-23 AT AT04078493T patent/ATE441460T1/en active
- 2004-12-23 ES ES04078493T patent/ES2330936T3/en active Active
- 2004-12-23 EP EP04078493A patent/EP1674129B1/en not_active Not-in-force
-
2005
- 2005-12-01 AU AU2005239691A patent/AU2005239691A1/en not_active Abandoned
- 2005-12-13 US US11/299,891 patent/US7542545B2/en not_active Expired - Fee Related
- 2005-12-22 JP JP2005370530A patent/JP4936723B2/en not_active Expired - Fee Related
- 2005-12-22 CA CA002531467A patent/CA2531467A1/en not_active Abandoned
Also Published As
Publication number | Publication date |
---|---|
ES2330936T3 (en) | 2009-12-17 |
DE602004022964D1 (en) | 2009-10-15 |
JP4936723B2 (en) | 2012-05-23 |
AU2005239691A1 (en) | 2006-07-13 |
PT1674129E (en) | 2009-11-17 |
JP2006175239A (en) | 2006-07-06 |
PL1674129T3 (en) | 2010-02-26 |
EP1674129A1 (en) | 2006-06-28 |
US7542545B2 (en) | 2009-06-02 |
ATE441460T1 (en) | 2009-09-15 |
US20060203964A1 (en) | 2006-09-14 |
DK1674129T3 (en) | 2009-11-23 |
EP1674129B1 (en) | 2009-09-02 |
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EEER | Examination request | ||
FZDE | Discontinued |
Effective date: 20131224 |