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8th Interventional MRI Symposium Book of Abstracts - Otto-von ...

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V-11<br />

Kalman-filtered velocity navigator triggering for motion<br />

compensated PRF thermometry<br />

F. Maier 1 , A. J. Krafft 1 , J. W. Jenne 2,3 , R. Dillmann 4 , W. Semmler 1 , M. Bock 1<br />

1<br />

Medical Physics in Radiology and 2 Clinical Cooperation Unit Radiation Oncology,<br />

German Cancer Research Center (DKFZ), Heidelberg, Germany<br />

3<br />

Mediri GmbH, Heidelberg, Germany<br />

4<br />

Institute <strong>of</strong> Anthropomatics, Karlsruhe Institute <strong>of</strong> Technology, Karlsruhe, Germany<br />

Objective<br />

For thermal therapies such as radio frequency, laser or focused ultrasound ablation<br />

thermometry is required. The preferred thermometry methods are non-invasive MR<br />

temperature measurements. In the most commonly applied proton resonance frequency (PRF)<br />

shift thermometry, temperature changes are calculated based on phase differences with<br />

respect to a reference. Since PRF thermometry is very sensitive to inter scan motion, this<br />

method is prone to motion artifacts. In the treatment <strong>of</strong> abdominal organs such as liver or<br />

kidney, breathing motion causes large tissue displacements. Different approaches have been<br />

proposed to address this problem. Triggered pulse sequences synchronize image acquisition to<br />

breathing motion [1-4], multi-baseline approaches acquire an atlas <strong>of</strong> reference images [3],<br />

and referenceless methods estimate the reference phase without a reference acquisition [5].<br />

Recently, a novel navigator technique for triggering MR thermometry image acquisition was<br />

presented [6]. In this work, an improved navigator acquisition was proposed. Additionally, the<br />

quality <strong>of</strong> the navigator signal was enhanced by Kalman filtering.<br />

Materials and Methods<br />

All experiments were carried out on a clinical 1.5 T whole body MR system<br />

(Magnetom Symphony, Siemens, Erlangen, Germany). The filtering and trigger algorithm<br />

was implemented directly on the image reconstruction system <strong>of</strong> the MR scanner.<br />

Pulse Sequence - A segmented EPI sequence (parameters: TR/TE = 25/15 ms, =<br />

18°, FOV: 298×216 mm, matrix: 128×92, slice thickness: 5 mm, EPI factor: 11, acquisition<br />

time per slice: 225 ms) was modified for triggered temperature mapping (Fig. 1). A bipolar<br />

gradient was inserted after slice selection and subsequently a navigator ADC without spatial<br />

encoding was acquired prior to the start <strong>of</strong> the readout train and the phase encoding gradients.<br />

Since the echo times <strong>of</strong> thermometry sequences are relatively long, the additional navigator<br />

gradients did not lead to a lengthening <strong>of</strong> TR. Until a trigger event was generated to start the<br />

acquisition <strong>of</strong> a complete slice (cf. trigger algorithm below), the first segment was acquired<br />

repeatedly to maintain magnetization steady state for subsequent image acquisition. The<br />

bipolar gradient was inverted for every second acquisition <strong>of</strong> the EPI echo train. Therefore, an<br />

increased total velocity sensitivity <strong>of</strong> VENC = 0.15 m/s could be realized. Velocity encoding<br />

can be applied in readout, phase encoding and slice selection direction. After a trigger event,<br />

velocity encoding was automatically disabled during image acquisition.<br />

Trigger Algorithm - Each navigator ADC measured eight complex signal values<br />

within 20 s, which were averaged. The phase <strong>of</strong> the values was unwrapped over time.<br />

Velocity was calculated by using the current velocity encoded navigator value and its<br />

inversely encoded predecessor (temporal distance: 1 × TR = 25 ms). A Kalman filter (cf.<br />

below) was applied to reduce noise and remove pulsation without a considerable temporal<br />

44

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