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Quantitative MR thermometry based on phase-drift correction PRF shift method at 0.35 T.
Chen, Yuping; Ge, Mengke; Ali, Rizwan; Jiang, Hejun; Huang, Xiaoyan; Qiu, Bensheng.
  • Chen Y; Centers for Biomedical Engineering, University of Science and Technology of China, Hefei, 230026, Anhui, China.
  • Ge M; Centers for Biomedical Engineering, University of Science and Technology of China, Hefei, 230026, Anhui, China.
  • Ali R; Centers for Biomedical Engineering, University of Science and Technology of China, Hefei, 230026, Anhui, China.
  • Jiang H; Centers for Biomedical Engineering, University of Science and Technology of China, Hefei, 230026, Anhui, China.
  • Huang X; Centers for Biomedical Engineering, University of Science and Technology of China, Hefei, 230026, Anhui, China.
  • Qiu B; Centers for Biomedical Engineering, University of Science and Technology of China, Hefei, 230026, Anhui, China. bqiu@ustc.edu.cn.
Biomed Eng Online ; 17(1): 39, 2018 Apr 10.
Article en En | MEDLINE | ID: mdl-29631576
ABSTRACT

BACKGROUND:

Noninvasive magnetic resonance thermometry (MRT) at low-field using proton resonance frequency shift (PRFS) is a promising technique for monitoring ablation temperature, since low-field MR scanners with open-configuration are more suitable for interventional procedures than closed systems. In this study, phase-drift correction PRFS with first-order polynomial fitting method was proposed to investigate the feasibility and accuracy of quantitative MR thermography during hyperthermia procedures in a 0.35 T open MR scanner.

METHODS:

Unheated phantom and ex vivo porcine liver experiments were performed to evaluate the optimal polynomial order for phase-drift correction PRFS. The temperature estimation approach was tested in brain temperature experiments of three healthy volunteers at room temperature, and in ex vivo porcine liver microwave ablation experiments. The output power of the microwave generator was set at 40 W for 330 s. In the unheated experiments, the temperature root mean square error (RMSE) in the inner region of interest was calculated to assess the best-fitting order for polynomial fit. For ablation experiments, relative temperature difference profile measured by the phase-drift correction PRFS was compared with the temperature changes recorded by fiber optic temperature probe around the microwave ablation antenna within the target thermal region.

RESULTS:

The phase-drift correction PRFS using first-order polynomial fitting could achieve the smallest temperature RMSE in unheated phantom, ex vivo porcine liver and in vivo human brain experiments. In the ex vivo porcine liver microwave ablation procedure, the temperature error between MRT and fiber optic probe of all but six temperature points were less than 2 °C. Overall, the RMSE of all temperature points was 1.49 °C.

CONCLUSIONS:

Both in vivo and ex vivo experiments showed that MR thermometry based on the phase-drift correction PRFS with first-order polynomial fitting could be applied to monitor temperature changes during microwave ablation in a low-field open-configuration whole-body MR scanner.
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Texto completo: 1 Banco de datos: MEDLINE Asunto principal: Imagen por Resonancia Magnética / Termometría Límite: Animals Idioma: En Año: 2018 Tipo del documento: Article

Texto completo: 1 Banco de datos: MEDLINE Asunto principal: Imagen por Resonancia Magnética / Termometría Límite: Animals Idioma: En Año: 2018 Tipo del documento: Article