Reliable estimation of PET attenuation coefficient (AC) is a fundamental problem in PET/MR imaging. Accurate measurement of bone density variation is vital to generate reliable subject-specific AC maps using MR. Also, minimizing the data acquisition time of MR sequences for AC is essential to allow more MR scans in a single PET/MR scanning session. In this work, we propose a new acquisition scheme combining UTE and multi-echo radial acquisition to reliably estimate the composition of water,
All experiments were performed on a whole-body PET-MR scanner (mMR, Siemens Healthcare, Erlangen, Germany) using head coil for both transmission and signal reception. A healthy volunteer was scanned using the proposed 3D UTE multi-echo radial sequence (Fig.1). The study protocol was approved by our local Institutional Review Board (IRB). The imaging parameters were: field-of-view (FOV) = 240$$$\times$$$240$$$\times$$$240 $$$mm^3$$$, matrix size = 128$$$\times$$$128$$$\times$$$128, TR = 9.9 $$$ms$$$, TE1/TE2/TE3/TE4/TE5/TE6/TE7 = 70/2110/2810/3550/4250/4990/5690 $$$\mu s$$$, hard pulse duration = 100 $$$\mu s$$$, gradient ramp time = 400 $$$\mu s$$$ (gradient slew rate = 48.9 $$$mT/m/ms$$$), plateau gradient amplitude = 19.57 $$$mT/m$$$, dwell time = 2.5 $$$\mu s$$$, number of TR units = 6434 (corresponding to acceleration factor of 8), and total scan time = ~1 $$$min$$$. A separate calibration scan was acquired from a water phantom to correct the k-space trajectory for each echo using a method similarly described previously [16]. Image reconstruction was performed using SENSE reconstruction [17,18] and non-uniform fast Fourier transform (NUFFT) reconstruction [19].
The composition of water and fat signals were jointly estimated as follows [20]:
$$\left\{\hat{\rho}_W,\hat{\rho}_F,\hat{R}_2^*,\triangle\hat{\omega}_0\right\}=arg\min_{\rho_W,\rho_F,R_2^*,\triangle \omega_0} \sum_{q=1}^Q\sum_{p=1}^P\mid I_q(TE_p) - (\rho_{W,q}+\rho_{F,q}\sum_{m=1}^M \alpha_m e^{-i\cdot \omega_m\cdot TE_p})\cdot e^{-TE_p\cdot R_{2,q}^*} \cdot e^{-i\cdot \triangle\omega_{0,q}\cdot TE_p} \mid^2 +\mu\sum_{q=1}^Q V(\rho_{W,q},\rho_{F,q},R_{2,q}^*,\triangle \omega_{0,q})$$
where $$$I_q(TE_p)$$$ denotes the signal at voxel $$$q = 1,…,Q$$$ and echo time $$$p=1,…7$$$, $$$\rho_{W,q}$$$ and $$$\rho_{F,q}$$$ denote the proton density signals from water and fat, respectively, $$$R_{2,q}^*$$$ denotes the single, representative relaxation rate of both water and fat, $$$\alpha_m$$$ and $$$\omega_m$$$ each denote the relative amplitudes (i.e., $$$\sum_{m=1}^M \alpha_m =1$$$) and frequency offsets of an M-peak (i.e., $$$M=6$$$) fat model [21], $$$\triangle\omega_{0,q}$$$ denotes the frequency offset due to magnetic field inhomogeneity ($$$\triangle B_0$$$), $$$\mu$$$ denotes the regularization parameter, and $$$V$$$ denotes a regularization function reflecting prior information. Subsequently, $$$\rho_W$$$ and $$$\rho_F$$$ were compared for image segmentation into water, fat, and bone components.
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