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V Casanova Borca

Publications and source records attributed to V Casanova Borca.

4 recordsLinked to original sources

Fitting late rectal bleeding data using different NTCP models: results from an Italian multi-centric study (AIROPROS0101).

BACKGROUND AND PURPOSE: Recent investigations demonstrated a significant correlation between rectal dose-volume patterns and late rectal toxicity. The reduction of the DVH to a value expressing the probability of complication would be suitable. To fit different normal tissue complication probability (NTCP) models to clinical outcome on late rectal bleeding after external beam radiotherapy (RT) for prostate cancer. PATIENTS AND METHODS: Rectal dose-volume histograms of the rectum (DVH) and clinical records of 547 prostate cancer patients (pts) pooled from five institutions previously collected and analyzed were considered. All patients were treated in supine position with 3 or 4-field techniques: 123 patients received an ICRU dose between 64 and 70 Gy, 255 patients between 70 and 74 Gy and 169 patients between 74 and 79.2 Gy; 457/547 patients were treated with conformal RT and 203/547 underwent radical prostatectomy before RT. Minimum follow-up was 18 months. Patients were considered as bleeders if showing grade 2/3 late bleeding (slightly modified RTOG/EORTC scoring system) within 18 months after the end of RT. Four NTCP models were considered: (a) the Lyman model with DVH reduced to the equivalent uniform dose (LEUD, coincident with the classical Lyman-Kutcher-Burman, LKB, model), (b) logistic with DVH reduced to EUD (LOGEUD), (c) Poisson coupled to EUD reduction scheme and (d) relative seriality (RS). The parameters for the different models were fit to the patient data using a maximum likelihood analysis. The 68% confidence intervals (CI) of each parameter were also derived. RESULTS: Forty six out of five hundred and forty seven patients experienced grade 2/3 late bleeding: 38/46 developed rectal bleeding within 18 months and were then considered as bleeders The risk of rectal bleeding can be well calculated with a 'smooth' function of EUD (with a seriality parameter n equal to 0.23 (CI 0.05), best fit result). Using LEUD the relationship between EUD and NTCP can be described with a TD50 of 81.9 Gy (CI 1.8 Gy) and a steepness parameter m of 0.19 (CI 0.01); when using LOGEUD, TD50 is 82.2 Gy and k is 7.85. Best fit parameters for RS are s=0.49, gamma=1.69, TD50=83.1 Gy. Qualitative as well as quantitative comparisons (chi-squared statistics, P=0.005) show that the models fit the observed complication rates very well. The results found in the overall population were substantially confirmed in the subgroup of radically treated patients (LEUD: n=0.24 m=0.14 TD50=75.8 Gy). If considering just the grade 3 bleeders (n=9) the best fit is found in correspondence of a n-value around 0.06, suggesting that for severe bleeding the rectum is more serial. CONCLUSIONS: Different NTCP models fit quite accurately the considered clinical data. The results are consistent with a rectum 'less serial' than previously reported investigations when considering grade 2 bleeding while a more serial behaviour was found for severe bleeding. EUD may be considered as a robust and simple parameter correlated with the risk of late rectal bleeding.

Combined Modality Therapy↗

[Physical-dosimetric characterization of a multi-leaf collimator system for clinical implementation in conformational radiotherapy].

INTRODUCTION: In the present paper we discuss the main dosimetric characteristics of the multileaf collimator (MLC) installed on the Elekta SLi Precise accelerators. To evaluate the effectiveness of the MLC in conformal radiotherapy, beam transmission through leaves and/or diaphragms, leakage between the leaves, central axis depth dose, surface dose, effective penumbra, scalopping effect and field size factors were measured. MATERIALS AND METHODS: The MLC installed on the dual energy (4 and 6 MV) linear accelerator Elekta SLi Precise consists of 40 opposed pairs of 75 mm thick tungsten leaves, set in two raws mounted in place of the upper collimator. Each leaf has a nominal projected width of 10 mm. The maximum field size attainable is 40 x 40 cm2 at 100 cm SAD. Beam transmission through leaves and/or diaphragms and field size factors were measured in RW3 phantom with a ionization chamber, leakage between the leaves and effective penumbra were instead evaluated with radiographic films (X-Omat-V) and a laser scanning photodensitometer. Percentage depth doses were measured in an automatic water phantom. RESULTS: For both energies, approximately 1% of the incident radiation on the multileaf collimator is transmitted through the backup collimator, while the transmission through the different combinations of leaves and collimators is between 0.03 and 0.14%. These values show a good agreement with literature data and are in general lower than the peak values specified by the manufacturer. The peak value of the leakage between the leaves was about 2% for both energies, without significative variation with gantry or collimator angle or distance from the axis. MLC shaped fields show a skin dose less (about 3%) than the one of cerrobend block shaped fields, because of the electronic contamination due to the plexiglass tray of the cerrobend blocks; in both cases, the depth doses are similar, as are flatness and symmetry of irradiation fields. The effective penumbra increases with field dimension, depth and leaves positioning, with a mean value of about 9 mm for both energies. The different beam configurations do not significantly affect the values of the field size factors. CONCLUSIONS: The dosimetric characteristics and the case of use of the Elekta multileaf collimator make its application to conformal radiotherapy convenient and reliable, able to improve the accuracy and the effectiveness of radiation therapy and to develop new kinds of treatments. However, because of the complexity of the MLC, its implementation in radiotherapic practice requires careful dosimetric characterization to evaluate those parameters (transmission, penumbra and output factors) that play a fundamental role in the accuracy of the treatment.

Equipment Design↗

[A quality control test of the image obtained with electronic portal imaging devices].

INTRODUCTION: A quality control of the digital image obtained from two electronic portal imaging devices is discussed. The devices are used to verify the radiotherapic treatment setup by comparing online images of the irradiated volume with those of the simulation devices. MATERIAL AND METHODS: Both iView and Target View devices, respectively installed on a dual energy SLi Precise Elekta and Saturne 42 Ge linear accelerators, consist of highly efficient phosphor screen and high quality videocamera, controlled by a workstation, able to generate digital portal images from few cGy doses. A phantom and software package are used to assess the spatial resolution and signal to noise ratio, and to compare tha data obtained. Spatial resolution and signal to noise ratio of both systems were studied as a function of energy, gantry angle and image acquisition parameters. RESULTS: The mean spatial resolutions obtained from the first 30 measurements were 0,265+/-0,012 and 0,220+/-0,010 lp/mm respectively for 6 and 18 MV of Saturne 42 (Target View) and 0,241+/-0,006 and 0,239+/-0,005 lp/mm for 4 and 6 MV of SLi (iView). Spatial resolution decreases as a function of energy, meanwhile there are no significant statistical differences as regards of the acquisition parameters; signal to noise ratio, instead, increases with integration time. Different values of the spatial resolution as a function of gantry angle are due to changes in the screen-camera distance and flexing of the detector housing. The quality control test is performed every 15 days by the technicians of our Radiotherapy Department. We set the reject level of spatial resolution and signal to noise ratio to be three standard deviations below the mean value obtained during the initial EPID characterization: if the measures fall below these values preventative maintenance is scheduled. CONCLUSIONS: The efficacy of the use electronic portal imaging devices for visualizing and quantifying the relative positions of anatomical structures within the radiation field depends on the image quality. It is therefore essential to devise quality control tests for the devices themselves, to guarantee an optimal level of system performance in a fast and efficient manner.

Equipment Design↗

Measurements of exit dose profiles in 60Co beams with a conventional portal film system.

An important step in the verification of the reliability of portal films as in vivo dosemeters is the evaluation of the agreement between exit dose profiles and optical density profiles measured on the portal film. To test the possibilities of a conventional portal film system in 60Co beams suitable for head and neck irradiation, we verified the agreement between relative exit doses (measured by ionization chamber) and relative optical densities, on cubic homogeneous phantoms, on an homogeneous "step" phantom and on a cubic phantom including air and aluminium inhomogeneities. The optical density profiles were corrected with the appropriate sensitometric curves. For an homogeneous phantom 10.8 cm thick and with the film in contact with the phantom, the agreement was found to be excellent with a mean deviation of 0.8% and a maximum deviation of 1.5%. The agreement was worse when the air gap between the exit surface of the phantom and the portal film was increased (with an air gap equal to 15 cm the maximum deviation was 4%), and when the thickness of the phantom was increased (for a thickness of 14.4 cm the maximum deviation was 3.1%). The agreement was found to be acceptable for the "step" phantom too, with a mean deviation around 1% and a maximum deviation within 2% (air gap equal to zero). When air and aluminium inhomogeneities were incorporated into the phantom a maximum deviation of 6% and a mean deviation less than 3% were found. Furthermore, the relative optical density profiles show an underestimate of measured off-axis exit dose values under a high density inhomogeneity and a small overestimate under a low density inhomogeneity. Results suggest the possibility of using conventional portal films for exit relative dosimetry in head and neck irradiation with 60Co beams if the air gap is kept as small as possible.

Air↗