mr thermometry
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2022 ◽  
Vol 39 (1) ◽  
pp. 108-119
Author(s):  
Ryan Holman ◽  
Laura Gui ◽  
Orane Lorton ◽  
Pauline Guillemin ◽  
Stéphane Desgranges ◽  
...  

Cancers ◽  
2021 ◽  
Vol 13 (22) ◽  
pp. 5617
Author(s):  
Kemal Sumser ◽  
Tomas Drizdal ◽  
Gennaro G. Bellizzi ◽  
Juan A. Hernandez-Tamames ◽  
Gerard C. van Rhoon ◽  
...  

Clinical effectiveness of hyperthermia treatments, in which tumor tissue is artificially heated to 40–44 °C for 60–90 min, can be hampered by a lack of accurate temperature monitoring. The need for noninvasive temperature monitoring in the head and neck region (H&N) and the potential of MR thermometry prompt us to design an MR compatible hyperthermia applicator: the MRcollar. In this work, we validate the design, numerical model, and MR performance of the MRcollar. The MRcollar antennas have low reflection coefficients (<−15 dB) and the intended low interaction between the individual antenna modules (<−32 dB). A 10 °C increase in 3 min was reached in a muscle-equivalent phantom, such that the specifications from the European Society for Hyperthermic Oncology were easily reached. The MRcollar had a minimal effect on MR image quality and a five-fold improvement in SNR was achieved using the integrated coils of the MRcollar, compared to the body coil. The feasibility of using the MRcollar in an MR environment was shown by a synchronous heating experiment. The match between the predicted SAR and measured SAR using MR thermometry satisfied the gamma criteria [distance-to-agreement = 5 mm, dose-difference = 7%]. All experiments combined show that the MRcollar delivers on the needs for MR—hyperthermia in the H&N and is ready for in vivo investigation.


Cancers ◽  
2021 ◽  
Vol 13 (14) ◽  
pp. 3503
Author(s):  
Iva VilasBoas-Ribeiro ◽  
Sergio Curto ◽  
Gerard C. van van Rhoon ◽  
Martine Franckena ◽  
Margarethus M. Paulides

The efficacy of a hyperthermia treatment depends on the delivery of well-controlled heating; hence, accurate temperature monitoring is essential for ensuring effective treatment. For deep pelvic hyperthermia, there are no comprehensive and systematic reports on MR thermometry. Moreover, data inclusion generally lacks objective selection criteria leading to a high probability of bias when comparing results. Herein, we studied whether imaging-based data inclusion predicts accuracy and could serve as a tool for prospective patient selection. The accuracy of the MR thermometry in patients with locally advanced cervical cancer was benchmarked against intraluminal temperature. We found that gastrointestinal air motion at the start of the treatment, quantified by the Jaccard similarity coefficient, was a good predictor for MR thermometry accuracy. The results for the group that was selected for low gastrointestinal air motion improved compared to the results for all patients by 50% (accuracy), 26% (precision), and 80% (bias). We found an average MR thermometry accuracy of 2.0 °C when all patients were considered and 1.0 °C for the selected group. These results serve as the basis for comprehensive benchmarking of novel technologies. The Jaccard similarity coefficient also has good potential to prospectively determine in which patients the MR thermometry will be valuable.


Author(s):  
Beatrice Lena ◽  
Lambertus W. Bartels ◽  
Cyril J. Ferrer ◽  
Chrit T. W. Moonen ◽  
Max A. Viergever ◽  
...  

PLoS ONE ◽  
2021 ◽  
Vol 16 (5) ◽  
pp. e0250636
Author(s):  
Marylène Delcey ◽  
Pierre Bour ◽  
Valéry Ozenne ◽  
Wadie Ben Hassen ◽  
Bruno Quesson

Purpose To propose a MR-thermometry method and associated data processing technique to predict the maximal RF-induced temperature increase near an implanted wire for any other MRI sequence. Methods A dynamic single shot echo planar imaging sequence was implemented that interleaves acquisition of several slices every second and an energy deposition module with adjustable parameters. Temperature images were processed in real time and compared to invasive fiber-optic measurements to assess accuracy of the method. The standard deviation of temperature was measured in gel and in vivo in the human brain of a volunteer. Temperature increases were measured for different RF exposure levels in a phantom containing an inserted wire and then a MR-conditional pacemaker lead. These calibration data set were fitted to a semi-empirical model allowing estimation of temperature increase of other acquisition sequences. Results The precision of the measurement obtained after filtering with a 1.6x1.6 mm2 in plane resolution was 0.2°C in gel, as well as in the human brain. A high correspondence was observed with invasive temperature measurements during RF-induced heating (0.5°C RMSE for a 11.5°C temperature increase). Temperature rises of 32.4°C and 6.5°C were reached at the tip of a wire and of a pacemaker lead, respectively. After successful fitting of temperature curves of the calibration data set, temperature rise predicted by the model was in good agreement (around 5% difference) with measured temperature by a fiber optic probe, for three other MRI sequences. Conclusion This method proposes a rapid and reliable quantification of the temperature rise near an implanted wire. Calibration data set and resulting fitting coefficients can be used to estimate temperature increase for any MRI sequence as function of its power and duration.


2021 ◽  
Vol 87 ◽  
pp. 101834
Author(s):  
B. Denis de Senneville ◽  
P. Coupé ◽  
M. Ries ◽  
L. Facq ◽  
C.T.W. Moonen
Keyword(s):  

2020 ◽  
Author(s):  
Andrew J. Fagan ◽  
Paul S. Jacobs ◽  
Thomas C. Hulshizer ◽  
Phillip J. Rossman ◽  
Matthew A. Frick ◽  
...  
Keyword(s):  

2020 ◽  
Vol 85 (3) ◽  
pp. 1282-1293
Author(s):  
Caroline Le Ster ◽  
Franck Mauconduit ◽  
Christian Mirkes ◽  
Michel Bottlaender ◽  
Fawzi Boumezbeur ◽  
...  

2020 ◽  
Vol 10 (9) ◽  
pp. 1823-1836
Author(s):  
Yangzi Qiao ◽  
Chao Zou ◽  
Chuanli Cheng ◽  
Changjun Tie ◽  
Qian Wan ◽  
...  

2020 ◽  
Vol 31 (8) ◽  
pp. 1357-1364
Author(s):  
Aaron W.P. Maxwell ◽  
William K.C. Park ◽  
Grayson L. Baird ◽  
Edward G. Walsh ◽  
Damian E. Dupuy

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