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  • 1
    In: Physics and Imaging in Radiation Oncology, Elsevier BV, Vol. 12 ( 2019-10), p. 56-62
    Type of Medium: Online Resource
    ISSN: 2405-6316
    Language: English
    Publisher: Elsevier BV
    Publication Date: 2019
    detail.hit.zdb_id: 2963795-8
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  • 2
    In: Medical Physics, Wiley, Vol. 46, No. 2 ( 2019-02), p. 1012-1023
    Abstract: Computed tomography ( CT ) is a versatile tool in diagnostic radiology with rapidly increasing number of examinations per year globally. Routine adaption of the exposure level for patient anatomy and examination protocol cause the patients' exposures to become diversified and harder to predict by simple methods. To facilitate individualized organ dose estimates, we explore the possibility to automate organ dose calculations using a radiotherapy treatment planning system ( TPS ). In particular, the mapping of CT number to elemental composition for Monte Carlo ( MC ) dose calculations is investigated. Methods Organ dose calculations were done for a female thorax examination test case with a TPS (Raystation™, Raysearch Laboratories AB , Stockholm, Sweden) utilizing a MC dose engine with a CT source model presented in a previous study. The TPS 's inherent tissue characterization model for mapping of CT number to elemental composition of the tissues was calibrated using a phantom with known elemental compositions and validated through comparison of MC calculated dose with dose measured with Thermo Luminescence Dosimeters ( TLD ) in an anthropomorphic phantom. Given the segmentation tools of the TPS , organ segmentation strategies suitable for automation were analyzed for high contrast organs, utilizing CT number thresholding and model‐based segmentation, and for low contrast organs utilizing water replacements in larger tissue volumes. Organ doses calculated with a selection of organ segmentation methods in combination with mapping of CT numbers to elemental composition ( RT model), normally used in radiotherapy, were compared to a tissue characterization model with organ segmentation and elemental compositions defined by replacement materials [International Commission on Radiological Protection ( ICRP ) model], frequently favored in imaging dosimetry. Results The results of the validation with the anthropomorphic phantom yielded mean deviations from the dose to water calculated with the RT and ICRP model as measured with TLD of 1.1% and 1.5% with maximum deviations of 6.1% and 8.7% respectively over all locations in the phantom. A strategy for automated organ segmentation was evaluated for two different risk organ groups, that is, low contrast soft organs and high contrast organs. The relative deviation between organ doses calculated with the RT model and with the ICRP model varied between 0% and 20% for the thorax/upper abdomen risk organs. Conclusions After calibration, the RT model in the TPS provides accurate MC dose results as compared to measurements with TLD and the ICRP model. Dosimetric feasible segmentation of the risk organs for a female thorax demonstrates a possibility for automation using the segmentation tool available in a TPS for high contrast organs. Low contrast soft organs can be represented by water volumes, but organ dose to the esophagus and thyroid must be determined using standardized organ shapes. The uncertainties of the organ doses are small compared to the overall uncertainty, at least an order of magnitude larger, in the estimates of lifetime attributable risk ( LAR ) based on organ doses. Large‐scale and automated individual organ dose calculations could provide an improvement in cancer incidence estimates from epidemiological studies.
    Type of Medium: Online Resource
    ISSN: 0094-2405 , 2473-4209
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2019
    detail.hit.zdb_id: 1466421-5
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  • 3
    In: Radiotherapy and Oncology, Elsevier BV, Vol. 182 ( 2023-05), p. 109539-
    Type of Medium: Online Resource
    ISSN: 0167-8140
    Language: English
    Publisher: Elsevier BV
    Publication Date: 2023
    detail.hit.zdb_id: 1500707-8
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  • 4
    In: Medical Physics, Wiley, Vol. 43, No. 11 ( 2016-11), p. 6118-6128
    Abstract: Radiation dose to patients undergoing examinations with Multislice Computed Tomography (MSCT) as well as Cone Beam Computed Tomography (CBCT) is a matter of concern. Risk management could benefit from efficient replace rational dose calculation tools. The paper aims to verify MSCT dose calculations using a Treatment Planning System (TPS) for radiotherapy and to evaluate four different variations of bow‐tie filter characterizations for the beam model used in the dose calculations. Methods A TPS (RayStation™, RaySearch Laboratories, Stockholm, Sweden) was configured to calculate dose from a MSCT (GE Healthcare, Wauwatosa, WI, USA). The x‐ray beam was characterized in a stationary position the by measurements of the Half‐Value Layer (HVL) in aluminum and kerma along the principal axes of the isocenter plane perpendicular to the beam. A Monte Carlo source model for the dose calculation was applied with four different variations on the beam‐shaping bow‐tie filter, taking into account the different degrees of HVL information but reconstructing the measured kerma distribution after the bow‐tie filter by adjusting the photon sampling function. The resulting dose calculations were verified by comparison with measurements in solid water as well as in an anthropomorphic phantom. Results The calculated depth dose in solid water as well as the relative dose profiles was in agreement with the corresponding measured values. Doses calculated in the anthropomorphic phantom in the range 26–55 mGy agreed with the corresponding thermo luminescence dosimeter (TLD) measurements. Deviations between measurements and calculations were of the order of the measurement uncertainties. There was no significant difference between the different variations on the bow‐tie filter modeling. Conclusions Under the assumption that the calculated kerma after the bow‐tie filter replicates the measured kerma, the central specification of the HVL of the x‐ray beam together with the kerma distribution can be used to characterize the beam. Thus, within the limits of the study, a flat bow‐tie filter with an HVL specified by the vendor suffices to calculate the dose distribution. The TPS could be successfully configured to replicate the beam movement and intensity modulation of a spiral scan with dose modulation, on the basis of the specifications available in the metadata of the digital images and the log file of the CT.
    Type of Medium: Online Resource
    ISSN: 0094-2405 , 2473-4209
    Language: English
    Publisher: Wiley
    Publication Date: 2016
    detail.hit.zdb_id: 1466421-5
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  • 5
    Online Resource
    Online Resource
    IOP Publishing ; 2021
    In:  Physics in Medicine & Biology Vol. 66, No. 18 ( 2021-09-21), p. 185015-
    In: Physics in Medicine & Biology, IOP Publishing, Vol. 66, No. 18 ( 2021-09-21), p. 185015-
    Abstract: Published data from cell survival experiments are frequently used as training data for models of proton relative biological effectiveness (RBE). The publications rarely provide full information about the primary particle spectrum of the used beam, or its content of heavy secondary particles. The purpose of this paper is to assess to what extent heavy secondary particles may have been present in published cell survival experiments, and to investigate the impact of non-primary protons for RBE calculations in treatment planning. We used the Monte Carlo code Geant4 to calculate the occurrence of non-primary protons and heavier secondary particles for clinical protons beams in water for four incident energies in the [100, 250] MeV interval. We used the resulting spectra together with a conservative RBE parameterization and an RBE model to map both the rise of RBE at the beam entry surface due to heavy secondary particle buildup, and the difference in estimated RBE if non-primary protons are included or not in the beam quality metric. If included, non-primary protons cause a difference of 2% of the RBE in the plateau region of an spread out Bragg peak and 1% in the Bragg peak. Including non-primary protons specifically for RBE calculations will consequently have a negligible impact and can be ign ored. A buildup distance in water of one millimeter was sufficient to reach an equilibrium state of RBE for the four incident energies selected. For the investigated experimental data, 83 out of the 86 data points were found to have been determined with at least that amount of buildup material. Hence, RBE model training data should be interpreted to include the contribution of heavy secondaries.
    Type of Medium: Online Resource
    ISSN: 0031-9155 , 1361-6560
    RVK:
    Language: Unknown
    Publisher: IOP Publishing
    Publication Date: 2021
    detail.hit.zdb_id: 1473501-5
    SSG: 12
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  • 6
    In: Acta Oncologica, Informa UK Limited, Vol. 60, No. 2 ( 2021-02-01), p. 199-206
    Type of Medium: Online Resource
    ISSN: 0284-186X , 1651-226X
    Language: English
    Publisher: Informa UK Limited
    Publication Date: 2021
    detail.hit.zdb_id: 1492623-4
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  • 7
    Online Resource
    Online Resource
    IOP Publishing ; 2007
    In:  Physics in Medicine and Biology Vol. 52, No. 11 ( 2007-06-01), p. 3151-3168
    In: Physics in Medicine and Biology, IOP Publishing, Vol. 52, No. 11 ( 2007-06-01), p. 3151-3168
    Type of Medium: Online Resource
    ISSN: 0031-9155 , 1361-6560
    RVK:
    Language: Unknown
    Publisher: IOP Publishing
    Publication Date: 2007
    detail.hit.zdb_id: 1473501-5
    SSG: 12
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  • 8
    In: Medical Physics, Wiley, Vol. 49, No. 5 ( 2022-05), p. 3444-3456
    Abstract: The primary objective of our study was to perform a quantitative robustness analysis of the dose‐averaged linear energy transfer (LET d ) and related RBE‐weighted dose in robustly optimized (in terms of the range and set up uncertainties) pencil beam scanning (PBS) proton lung cancer plans. Methods In this study, we utilized the 4DCT dataset of six anonymized lung patients. PBS lung plans were generated using a robust optimization technique (range uncertainty: ±3.5% and setup errors: ±5 mm) on the CTV for a total dose of 5000 cGy (RBE) in five fractions using the RBE of 1.1. For each patient, the LET d distributions were calculated for the nominal plan and three groups. Group 1 : two plan robustness scenarios for range uncertainties of ±3.5%; Group 2 : twelve plan robustness scenarios (range uncertainty (±3.5%) in conjunction with setup errors (±5 mm)); and Group 3 : ten different breathing phases of the 4DCT dataset. The RBE‐weighted dose to the OARs was evaluated for all robustness scenarios and breathing phases. The variation (∆) in the mean LET d and mean RBE‐weighted dose from each group was recorded. Results The mean LET d in the CTV of nominal PBS lung plans among six patients ranged from 2.2 to 2.6 keV/µm. On average, for the combined range and setup uncertainties, the ∆ in the mean LET d among 12 scenarios of all six patients was 0.6 keV/µm, which is slightly higher than when only the range uncertainties were considered (0.4 keV/µm). The ∆ in the mean LET d in a patient was ≤1.7 keV/µm in the heart and ≤1.2 keV/µm in the esophagus and total lung. The ∆ in the mean RBE‐weighted dose in a patient was up to 79 cGy for the total lung, 165 cGy for the heart, and 258 cGy for the esophagus. For ten breathing phases, the ∆ in the mean LET d in a patient was ≤0.3 keV/µm in the CTV, ≤0.5 keV/µm in the heart, ≤0.4 keV/µm in the esophagus, and ≤0.7 keV/µm in the total lung. Conclusion The addition of setup errors to the range uncertainties resulted in slightly less homogeneous LET d distributions. The variations in the mean LET d among the ten breathing phases were slightly larger in the total lung than in the heart and esophagus. The combination of setup and range uncertainties had a greater impact than the effect of breathing phases on the variations in the mean RBE‐weighted dose to the OARs. Overall, the LET d distributions in the CTV were less sensitive than those in the OARs to setup errors, range uncertainties, and breathing phases for robustly optimized (in terms of range and setup uncertainities) PBS proton lung cancer plans.
    Type of Medium: Online Resource
    ISSN: 0094-2405 , 2473-4209
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2022
    detail.hit.zdb_id: 1466421-5
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  • 9
    In: Medical Physics, Wiley
    Abstract: Large tumor size has been reported as a predicting factor for inferior clinical outcome in carbon ion radiotherapy (CIRT). Besides the clinical factors accompanied with such tumors, larger tumors receive typically more low linear energy transfer (LET) contributions than small ones which may be the underlying physical cause. Although dose averaged LET is often used as a single parameter descriptor to quantify the beam quality, there is no evidence that this parameter is the optimal clinical predictor for the complex mixed radiation fields in CIRT. Purpose Purpose of this study was to investigate on a novel dosimetric quantity, namely high‐LET‐dose (, the physical dose filtered based on an LET threshold) as a single parameter estimator to differentiate between carbon ion treatment plans (cTP) with a small and large tumor volume. Methods Ten cTPs with a planning target volume, (large) and nine with a (small) were selected for this study. To find a reasonable LET threshold () that results in a significant difference in terms of , the voxel based normalized high‐LET‐dose () distribution in the clinical target volume (CTV) was studied on a subset (12 out of 19 cTPs) for 18 LET thresholds, using standard distribution descriptors (mean, variance and skewness). The classical dose volume histogram concept was used to evaluate the and distributions within the target of all 19 cTPs at the before determined . Statistical significance of the difference between the two groups in terms of mean and volume histogram parameters was evaluated by means of (two‐sided) t ‐test or Mann‐Whitney‐ U ‐test. In addition, the minimum target coverage at the above determined was compared and validated against three other thresholds to verify its potential in differentiation between small and large volume tumors. Results An of approximately was found to be a reasonable threshold to classify the two groups. At this threshold, the and were significantly larger () in small CTVs. For the small tumor group, the near‐minimum and median (and ) in the CTV were in average (0.31 ± 0.08) and (0.46 ± 0.06), respectively. For the large tumors, these parameters were (0.20 ± 0.01) and (0.28 ± 0.02). The difference between the two groups in terms of mean near‐minimum and median () was 2.7 Gy (11%) and 5.0 Gy (18%), respectively. Conclusions The feasibility of high‐LET‐dose based evaluation was shown in this study where a lower was found in cTPs with a large tumor size. Further investigation is needed to draw clinical conclusions. The proposed methodology in this work can be utilized for future high‐LET‐dose based studies.
    Type of Medium: Online Resource
    ISSN: 0094-2405 , 2473-4209
    Language: English
    Publisher: Wiley
    Publication Date: 2023
    detail.hit.zdb_id: 1466421-5
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  • 10
    In: Radiation Oncology, Springer Science and Business Media LLC, Vol. 17, No. 1 ( 2022-10-22)
    Abstract: To introduce and compare multiple biological effectiveness guided (BG) proton plan optimization strategies minimizing variable relative biological effectiveness (RBE) induced dose burden in organs at risk (OAR) while maintaining plan quality with a constant RBE. Methods Dose-optimized (DOSEopt) proton pencil beam scanning reference treatment plans were generated for ten cranial patients with prescription doses ≥ 54 Gy(RBE) and ≥ 1 OAR close to the clinical target volume (CTV). For each patient, four additional BG plans were created. BG objectives minimized either proton track-ends, dose-averaged linear energy transfer (LET d ), energy depositions from high-LET protons or variable RBE-weighted dose (D RBE ) in adjacent serially structured OARs. Plan quality (RBE = 1.1) was assessed by CTV dose coverage and robustness (2 mm setup, 3.5% density), dose homogeneity and conformity in the planning target volumes and adherence to OAR tolerance doses. LET d , D RBE (Wedenberg model, α/β CTV  = 10 Gy, α/β OAR  = 2 Gy) and resulting normal tissue complication probabilities (NTCPs) for blindness and brainstem necrosis were derived. Differences between DOSEopt and BG optimized plans were assessed and statistically tested (Wilcoxon signed rank, α = 0.05). Results All plans were clinically acceptable. DOSEopt and BG optimized plans were comparable in target volume coverage, homogeneity and conformity. For recalculated D RBE in all patients, all BG plans significantly reduced near-maximum D RBE to critical OARs with differences up to 8.2 Gy(RBE) ( p   〈  0.05). Direct D RBE optimization primarily reduced absorbed dose in OARs (average ΔD mean  = 2.0 Gy; average ΔLET d,mean  = 0.1 keV/µm), while the other strategies reduced LET d (average ΔD mean   〈  0.3 Gy; average ΔLET d,mean  = 0.5 keV/µm). LET-optimizing strategies were more robust against range and setup uncertaintes for high-dose CTVs than D RBE optimization. All BG strategies reduced NTCP for brainstem necrosis and blindness on average by 47% with average and maximum reductions of 5.4 and 18.4 percentage points, respectively. Conclusions All BG strategies reduced variable RBE-induced NTCPs to OARs. Reducing LET d in high-dose voxels may be favourable due to its adherence to current dose reporting and maintenance of clinical plan quality and the availability of reported LET d and dose levels from clinical toxicity reports after cranial proton therapy. These optimization strategies beyond dose may be a first step towards safely translating variable RBE optimization in the clinics.
    Type of Medium: Online Resource
    ISSN: 1748-717X
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2022
    detail.hit.zdb_id: 2224965-5
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