Accelerated MR-Based Motion Field Measurement for PET Motion Correction in PET/MR

Background: The intrinsic resolution of modern whole-body PET scanners is about 4 mm, but the practically achievable resolution of thoracic or abdominal PET imaging may be worse than 10 mm due to inevitable cardiac and respiratory motion. PET/MR provides a unique opportunity to address this issue by...

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Bibliographic Details
Published inThe Journal of nuclear medicine (1978) Vol. 60
Main Authors Han, Paul, Djebra, Yanis, Petibon, Yoann, Marin, Thibault, Ouyang, Jinsong, El Fakhri, Georges, Ma, Chao
Format Journal Article
LanguageEnglish
Published New York Society of Nuclear Medicine 01.05.2019
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Summary:Background: The intrinsic resolution of modern whole-body PET scanners is about 4 mm, but the practically achievable resolution of thoracic or abdominal PET imaging may be worse than 10 mm due to inevitable cardiac and respiratory motion. PET/MR provides a unique opportunity to address this issue by taking advantage of the high-resolution images with excellent soft-tissue contrasts offered by MR. In the past, MR-based motion field measurement methods have been developed and used to improve the resolution of PET in free-breathing patients. However, these methods often require cardiac and/or respiratory gating and long data acquisition times, limiting their use in clinical applications. This work presents a subspace-based method to accelerate the imaging speed of MR-based motion field measurement for PET motion correction in PET/MR. Methods: Our method leverages a unique property of dynamic MR images, known as partial separability [1], to accelerate the imaging speed of MR-based motion field measurement. We represent a dynamic MR dataset as partially separable (PS) functions: The true signal ρ(x,t) is expressed as the sum of Ul(x)Vl(t) as l goes from 1 to L, where Vl(t) are the temporal basis functions capturing the underlying dynamics of the data, Ul(x) are the corresponding spatial coefficients determining the spatial distributions of the data, and L is the model order (a small number in practice). The PS model indicates that the high-dimensional dynamic MR images reside in a low-dimensional subspace, which significantly reduces the number of degrees of freedom of the data. Furthermore, it enables a special data acquisition scheme (as shown in Fig.1A) for sparse sampling, where two datasets are acquired in an interleaved fashion: a low-resolution "training" dataset to determine the temporal bases Vl(t) and a sparsely sampled "imaging" dataset to estimate the spatial bases Ul(x). The image reconstruction is done by fitting the PS model to the measured k-space data. To validate the performance of the proposed method, we performed MR scan on healthy volunteers (approved by our local IRB) on a whole-body MR scanner (Trio, Siemens Healthcare, Erlangen, Germany). The imaging parameters are as follows: field-of-view (FOV)=360×304×120 mm3, resolution=1.875×1.875×5 mm, TR/TE=4/2 ms, total acquisition time = ~5 min. Free-breathing continuous MR acquisition without any gating was performed as shown in Fig.1A. Results: Representative reconstruction results are shown in Fig.1B. Images were reconstructed using the proposed method and the conventional sliding window methods, respectively, with a frame rate of 0.22 s/frame. Our method produced high-quality dynamic 3D MR images without noticeable motion artifacts as compared to the sliding window method. Note that only 44 phase-encoding lines were acquired per frame, which translates to 1.13% of the fully sampled data at the Nyquist rate. Conclusions: The partially separable model can be used to accelerate the imaging speed of MR-based motion field method. The proposed method can improve the practical utility of MR-based motion correction of PET in PET/MR.
ISSN:0161-5505
1535-5667