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Background: The improvement of in vitro assessment of targeted alpha therapy (reproducibility, comparability of experiments...) requires precise evaluation of the dose delivered to the cells. To answer this need, a previous study proposed an innovative dosimetry method based on α‐spectroscopy and a specific deconvolution process to recover the spatial distribution of 212Pb isotopes inside in vitro culture wells. Nevertheless, although promising, the deconvolution method was time consuming and only tested for a simple isotope decay chain. Purpose: The purpose of this work is to propose a new matrix deconvolution method of α spectra based on a constrained‐non‐negative‐maximum‐likelihood decomposition, both faster and offering a greater modelling flexibility, allowing to study independently the kinetics of each of the daughter nuclides of complex decay chains (illustrated here with 223Ra) in in vitro culture wells. Methods: Firstly, the performance of the new method was fully evaluated through Monte Carlo simulations of in vitro irradiations. Different spatial distributions of 212Pb and 223Ra, the corresponding α spectra measured by a silicon detector and the doses delivered to the cells were simulated with Geant4. The deconvolution results were then compared to the simulation results. Secondly, measurements were carried out in culture wells without cells containing 15 kBq of 212Pb or 9.3 kBq of 223Ra, placed above silicon detectors recording α spectra in real time. The matrix deconvolution was then applied to determine the spatial and temporal distribution of all α‐emitting daughters of studied isotopes. Results: The matrix deconvolution was proved to recover the simulated distribution gradients, ensuring simulated doses within 3 % for both tested radionuclides, with errors on dose normally distributed around the reference value (consequently not exhibiting any bias), even in the case of complex decay chains as 223Ra. The experimental study of 212Pb and 223Ra showed highly inhomogeneous distributions and time evolution of the concentration gradients, consistent with the previous study. Furthermore, it highlighted the complex kinetics of 223Ra with different distributions of its α‐emitting daughters (219Rn, 215Po, 215At, 211Bi, 211Po). Conclusions: This study validates a new deconvolution method, fast and flexible, that proved to be accurate and reliable. This method allowed to reveal the complexity of isotopes kinetics in in vitro experiments, especially with complex decay chains. Experimental dosimetry, necessary to improve reliability of in vitro studies in targeted alpha therapy, is demonstrated to be feasible with the proposed method. [ABSTRACT FROM AUTHOR]

Acute ischemic stroke results in an ischemic core surrounded by a tissue at risk, named the penumbra, which is potentially salvageable. One way to differentiate the tissues is to measure the hypoxia status. The purpose of the current study is to correlate the abnormal brain tissue volume derived from magnetic resonance‐based imaging of brain oxygen saturation (StO2‐MRI) to the fluorine‐18 fluoromisonidazole ([18F]FMISO) positron emission tomography (PET) volume for hypoxia imaging validation, and to analyze the ability of StO2‐MRI to depict the different hypoxic tissue types in the acute phase of stroke. In a pertinent model of stroke in the rat, the volume of tissue with decreased StO2‐MRI signal and that with increased uptake of [18F]FMISO were equivalent and correlated (r = 0.706; p = 0.015). The values of StO2 in the tissue at risk were significantly greater than those quantified in the core of the lesion, and were less than those for healthy tissue (52.3% ± 2.0%; 43.3% ± 1.9%, and 67.9 ± 1.4%, respectively). A threshold value for StO2 of ≈60% as the cut‐off for the identification of the tissue at risk was calculated. Tissue volumes with reduced StO2‐MRI correlated with the final lesion (r = 0.964, p < 0.0001). The findings show that the StO2‐MRI approach is sensitive for the detection of hypoxia and for the prediction of the final lesion after stroke. Once validated in acute clinical settings, this approach might be used to enhance the stratification of patients for potential therapeutic interventions. [ABSTRACT FROM AUTHOR]

Purpose: Targeted alpha therapy (TAT) takes advantage of the short‐range and high‐linear energy transfer of α‐particles and is increasingly used, especially for the treatment of metastatic lesions. Nevertheless, dosimetry of α‐emitters is challenging for the very same reasons, even for in vitro experiments. Assumptions, such as the uniformity of the distribution of radionuclides in the culture medium, are commonly made, which could have a profound impact on dose calculations. In this study we measured the spatial distribution of α‐emitting 212Pb coupled to an anti‐VCAM‐1 antibody (212Pb‐αVCAM‐1) and its evolution over time in the context of in vitro irradiations. Methods: Two experimental setups were implemented without cells to measure α‐particle count rates and energy spectra in culture medium containing 15 kBq of 212Pb‐α‐VCAM‐1. Silicon detectors were placed above and below cell culture dishes for 20 h. One of the dishes had a 2.5‐µm‐thick mylar‐base allowing easy detection of the α‐particles. Monte Carlo simulations were performed to analyze experimental spectra. Experimental setups were modeled and α‐energy spectra were simulated in the silicon detectors for different decay positions in the culture medium. Simulated spectra were then used to deconvolute experimental spectra to determine the spatial distribution of 212Pb‐αVCAM‐1 in the medium. This distribution was finally used to calculate the dose deposition in cell culture experiments. Results: Experimental count rates and energy spectra showed differences in measurements taken at the top and the bottom of dishes and temporal variations that did not follow 212Pb decay. The radionuclide spatial distribution was shown to be composed of a uniform distribution and concentration gradients at the top and the bottom, which were subjected to temporal variations that may be explained by gravity and electrostatic attraction. The absorbed dose in cells calculated from this distribution was compared with the dose expected for a uniform and static distribution and found to be 1.75 times higher, which is highly significant to interpret biological observations. Conclusions: This study demonstrated that accurate dosimetry of α‐emitters requires the experimental determination of radionuclide spatial and temporal distribution and highlighted that in vitro assessment of dose for TAT cannot only rely on a uniform distribution of activity in the culture medium. The reliability and reproducibility of future experiments should benefit from specifically developed dosimetry tools and methods. [ABSTRACT FROM AUTHOR]