Generating MRI-based pseudo-CT images, providing electron density information for dose calculation, is the first step towards MRI-based radiation therapy treatment planning. Existing methods either require prior knowledge of a CT-MR atlas or require acquisition of multiple scans. In this study, we demonstrated the feasibility of producing pseudo-CT images by using a single multi-gradient-echo sequence. This method takes advantage of tissue-specific relaxation properties of MRI signal to provided segmentation of bone, air and other anatomical structures. Since all images are generated from a single scan and are naturally co-registered, this method is fast and avoids registration errors.
This study was approved by local IRB and the subject provided informed consent. All MRI scans were collected using a 1.5T scanner (Ingenia, Philips Medical System) equipped with a 15-channel phased-array head coil. High resolution Gradient Echo Plural Contrast Imaging (GEPCI)1,2 datasets with a voxel size of $$$1\times1\times3mm^{3}$$$ were acquired using a 3D multi-gradient-echo sequence with a flip angle of $$$30^\circ$$$, $$$TR=50ms$$$ and total acquisition time of 7min. For each acquisition, 11 echoes were collected with $$$TE1=4ms$$$ and $$$\Delta TE=4ms$$$. Signals from different channels were combined for each voxel:
$$S(TE)=\frac{1}{M}\sum_{m=1}^M\lambda_{m}\overline{S}(TE_{1})S_{m}(TE_{n})$$
$$\lambda_{m}=\frac{1}{M}\sum_{l=1}^{M}\frac{\sigma_{l}^{2}}{\sigma_{m}^{2}}$$
where the sum is taken over all channels (m), $$$\overline S$$$ denotes complex conjugate of S, $$$\lambda_{m}$$$ are weighting parameters and $$$\sigma_{m}$$$ are noise amplitudes (r.m.s.). We omit index corresponding to voxel position for clarity. This algorithm allows for the optimal estimation of quantitative parameters, such as magnetic resonance signal magnitude, decay rate constant and frequency and also removes the initial phase incoherence between channels2. R2* constants were obtained by fitting the channel-combined data on a voxel-by-voxel basis:
$$S(TE)=S_{0}^{2}\cdot e^{-R_{2}^{*}\cdot (TE+TE_{1})}\cdot e^{i\cdot\omega\cdot(TE-TE_{1})}\cdot F(TE)$$
where $$$\omega$$$ is a local signal frequency and F(TE) is the F-function describing the influence of macroscopic magnetic field inhomogeneity effects on MRI signal. Herein, we use a voxel spread function algorithm3 for evaluation of F-function.
TRD-CT images were created as described in Fig.1. Magnitude images of the first echo ($$$I(TE_{1})$$$) were inverted ($$$1/I(TE_{1})$$$) to create positive enhanced contrasts of the “air” regions and to produce an “air” mask. Due to complex TE-dependent behavior of the MRI signal in fat-rich regions, the $$$\chi^{2}$$$ error of fitting the mono-exponential model to experimental data is much larger than in all other areas. The $$$\chi^{2}$$$ map was used to create a “fat” mask. R2* from the mono-exponential fitting using first 3 echoes was used to define “soft-tissue” as regions with low R2* values ($$$\leq50s^{-1}$$$). By applying air-, fat- and soft-tissue-mask to R2* map, the “bone” areas were highlighted and a “bone” mask was created. Different anatomical structures were assigned a single Hounsfield units value (-1000$$$\rightarrow$$$air, -75$$$\rightarrow$$$fat, 40$$$\rightarrow$$$soft tissue and 1000$$$\rightarrow$$$bone) to create a pseudo-CT.
Brain CT was acquired using a CT Simulator (Brilliance, Philips Medical System,) with 120kVp, 500mAs, $$$512\times 512$$$ in-plane dimensions, $$$0.88\times 0.88mm^{2}$$$ in-plane spatial resolution and 1.5mm slice thickness. The accuracy of bone segmentation from TRD-CT was determined by calculating the Sorensen-Dice coefficient:
$$C=\frac{2\cdot|TRD_{CT}\bigcap CT|}{|TRD_{CT}|+|CT|}$$
Voxels in CT that had numbers bigger than 500 HU were classified as bone areas. Voxels that had values smaller than -500 HU were classified as air.
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