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Yousuke Hara,
Yoshihisa Takada, Kenji Hotta,
Ryohei Tansho,
Tetsuya Nihei,
Yojiro Suzuki,
Kosuke Nagafuchi,
Ryuichi Kawai,
Masaki Tanabe,
Shohei Mizutani,
Takeshi Himukai,
Naruhiro Matsufuji
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ABSTRACT: We have developed a novel design method of ridge filters for carbon-ion therapy using a broad-beam delivery system to improve the flatness of a biologically effective dose in the spread-out Bragg peak (SOBP). So far, the flatness of the SOBP is limited to about ±5% for carbon beams since the weight control of component Bragg curves composing the SOBP is difficult. This difficulty arises from using a large number of ridge-bar steps (e.g. about 100 for a SOBP width of 60 mm) required to form the SOBP for the pristine Bragg curve with an extremely sharp distal falloff. Instead of using a single ridge filter, we introduce a ripple filter to broaden the Bragg peak so that the number of ridge-bar steps can be reduced to about 30 for SOBP with of 60 mm for the ridge filter designed for the broadened Bragg peak. Thus we can manufacture the ridge filter more accurately and then attain a better flatness of the SOBP due to well-controlled weights of the component Bragg curves. We placed the ripple filter on the same frame of the ridge filter and arranged the direction of the ripple-filter-bar array perpendicular to that of the ridge-filter-bar array. We applied this method to a 290 MeV u(-1) carbon-ion beam in Heavy Ion Medical Accelerator in Chiba and verified the effectiveness by measurements.
Physics in Medicine and Biology 03/2012; 57(6):1717-31. · 2.83 Impact Factor
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ABSTRACT: When in vivo proton dosimetry is performed with a metal-oxide semiconductor field-effect transistor (MOSFET) detector, the response of the detector depends strongly on the linear energy transfer. The present study reports a practical method to correct the MOSFET response for linear energy transfer dependence by using a simplified Monte Carlo dose calculation method (SMC). A depth-output curve for a mono-energetic proton beam in polyethylene was measured with the MOSFET detector. This curve was used to calculate MOSFET output distributions with the SMC (SMC(MOSFET)). The SMC(MOSFET) output value at an arbitrary point was compared with the value obtained by the conventional SMC(PPIC), which calculates proton dose distributions by using the depth-dose curve determined by a parallel-plate ionization chamber (PPIC). The ratio of the two values was used to calculate the correction factor of the MOSFET response at an arbitrary point. The dose obtained by the MOSFET detector was determined from the product of the correction factor and the MOSFET raw dose. When in vivo proton dosimetry was performed with the MOSFET detector in an anthropomorphic phantom, the corrected MOSFET doses agreed with the SMC(PPIC) results within the measurement error. To our knowledge, this is the first report of successful in vivo proton dosimetry with a MOSFET detector.
Journal of Applied Clinical Medical Physics 01/2012; 13(2):3699. · 1.29 Impact Factor
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ABSTRACT: We experimentally evaluated the proton beam dose reproducibility, sensitivity, angular dependence and depth-dose relationships for a new Metal Oxide Semiconductor Field Effect Transistor (MOSFET) detector. The detector was fabricated with a thinner oxide layer and was operated at high-bias voltages. In order to accurately measure dose distributions, we developed a practical method for correcting the MOSFET response to proton beams. The detector was tested by examining lateral dose profiles formed by protons passing through an L-shaped bolus. The dose reproducibility, angular dependence and depth-dose response were evaluated using a 190 MeV proton beam. Depth-output curves produced using the MOSFET detectors were compared with results obtained using an ionization chamber (IC). Since accurate measurements of proton dose distribution require correction for LET effects, we developed a simple dose-weighted correction method. The correction factors were determined as a function of proton penetration depth, or residual range. The residual proton range at each measurement point was calculated using the pencil beam algorithm. Lateral measurements in a phantom were obtained for pristine and SOBP beams. The reproducibility of the MOSFET detector was within 2%, and the angular dependence was less than 9%. The detector exhibited a good response at the Bragg peak (0.74 relative to the IC detector). For dose distributions resulting from protons passing through an L-shaped bolus, the corrected MOSFET dose agreed well with the IC results. Absolute proton dosimetry can be performed using MOSFET detectors to a precision of about 3% (1 sigma). A thinner oxide layer thickness improved the LET in proton dosimetry. By employing correction methods for LET dependence, it is possible to measure absolute proton dose using MOSFET detectors.
Journal of Applied Clinical Medical Physics 01/2011; 12(2):3431. · 1.29 Impact Factor
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ABSTRACT: Treatment planning for proton tumor therapy requires a fast and accurate dose-calculation method. We have implemented a simplified Monte Carlo (SMC) method in the treatment planning system of the National Cancer Center Hospital East for the double-scattering beam delivery scheme. The SMC method takes into account the scattering effect in materials more accurately than the pencil beam algorithm by tracking individual proton paths. We confirmed that the SMC method reproduced measured dose distributions in a heterogeneous slab phantom better than the pencil beam method. When applied to a complex anthropomorphic phantom, the SMC method reproduced the measured dose distribution well, satisfying an accuracy tolerance of 3 mm and 3% in the gamma index analysis. The SMC method required approximately 30 min to complete the calculation over a target volume of 500 cc, much less than the time required for the full Monte Carlo calculation. The SMC method is a candidate for a practical calculation technique with sufficient accuracy for clinical application.
Physics in Medicine and Biology 06/2010; 55(12):3545-56. · 2.83 Impact Factor
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ABSTRACT: A range compensator (abbreviated as a RC hereafter) is used to form a conformal dose distribution for heavy-charged-particle therapy. However, it induces distortion of the dose distribution. The induced inhomogeneity may result in a calibration error of a monitor unit (MU) assigned to a transmission ionization chamber. By using a bi-material RC made from a low-Z material and a high-Z material instead of the regular RC, the dose inhomogeneity has been obviously reduced by equalizing the lateral dose distributions formed by pencil beams traversing elements of the RC with different base thicknesses at the same water-equivalent depth. We designed and manufactured a 4 x 4 matrix-shaped single-material RC and a bi-material RC with the same range losses at corresponding elements of the RCs. The bi-material RC is made from chemical wood (the main chemical component is an ABS resin) as a low-Z material and from brass as a high-Z material. Sixteen segments of the RC are designed so that the range-loss differences of the adjacent segments of the RC range from 0 to 50 mm in steps of 5 mm. We measured dose distributions in water formed by a 160 MeV proton beam traversing the single-material RC or the bi-material RC, using the HIMAC biology beam port. Large dips and bumps were observed in the dose distribution formed by the use of the single-material RC; the dose uniformity has been significantly improved in the target region by the use of the bi-material RC. The improvement has been obtained at the expense of blurring lateral penumbra. For clinical application of this method to a patient with large density inhomogeneity, a simple modification method of the original calculation model has been given.
Physics in Medicine and Biology 11/2008; 53(19):5555-69. · 2.83 Impact Factor
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ABSTRACT: A novel design method of ridge filters (RFs) has been developed for general proton beam lines which use a single-radius beam wobbling method. It can be applied to beam lines that transport both protons and carbon ions which are about three times longer than regular beam lines dedicated to protons. We designed an RF with an SOBP (spread-out Bragg peak) width of 60 mm in water for the 160-MeV proton beam of the HIMAC (Heavy Ion Medical Accelerator in Chiba) biology beam line using an existing model of the RF. Yet we observed a slope in the SOBP region when we used the RF. To elucidate the source of the slope, we have developed a new calculation model taking into account the geometry of the RF and a beam-limiting device. The source for the slope was found to be the large scattering effect of protons in the RF and beam restriction by a ring collimator (aperture diameter: 160 mm) placed just before the RF. When both fluence reduction by the scattering effect of protons in the RF and the beam-collimation effect are taken into account, proper RFs can be designed universally for a given beam line arrangement using the single-radius beam-wobbling method from the start without any trial-and-error process. This will serve to reduce the commissioning time of newly designed beam delivery systems.
Igaku butsuri: Nihon Igaku Butsuri Gakkai kikanshi = Japanese journal of medical physics: an official journal of Japan Society of Medical Physics 01/2008; 28(2):57-69.
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ABSTRACT: The metal oxide semiconductor field-effect transistor (MOSFET) dosimeter has been widely studied for use as a dosimeter for patient dose verification. The major advantage of this detector is its size, which acts as a point dosimeter, and also its ease of use. The commercially available TN502RD MOSFET dosimeter manufactured by Thomson and Nielsen has never been used for proton dosimetry. Therefore we used the MOSFET dosimeter for the first time in proton dose measurements. In this study, the MOSFET dosimeter was irradiated with 190 MeV therapeutic proton beams. We experimentally evaluated dose reproducibility, linearity, fading effect, beam intensity dependence and angular dependence for the proton beam. Furthermore, the Bragg curve and spread-out Bragg peak were also measured and the linear-energy transfer (LET) dependence of the MOSFET response was investigated. Many characteristics of the MOSFET response for proton beams were the same as those for photon beams reported in previous papers. However, the angular MOSFET responses at 45, 90, 135, 225, 270 and 315 degrees for proton beams were over-responses of about 15%, and moreover the MOSFET response depended strongly on the LET of the proton beam. This study showed that the angular dependence and LET dependence of the MOSFET response must be considered very carefully for quantitative proton dose evaluations.
Physics in Medicine and Biology 01/2007; 51(23):6077-86. · 2.83 Impact Factor
