Novel diffusion weighted MRI pulse sequences based on reduced FOV (rFOV) and multi-shot echo-planar imaging (msEPI), respectively, have been proposed to reduce distortions present in standard single-shot EPI. In this study, the quantitative reproducibility of prostate diffusion measurements with rFOV and msEPI is investigated with healthy volunteers. Diffusion parameters were estimated from different sequences (ssEPI, rFOV, msEPI), b-value groups, and diffusion models (mono-exponential, stretched exponential and kurtosis). Measurements from rFOV and msEPI are in good agreement with the standard ssEPI, demonstrating reproducibility across pulse sequences.
Acquisitions: After IRB approval and informed written consent, six healthy volunteers were scanned with the lower coils of a 32-channel torso coil array on a 3T MR scanner (MR 750, GE Healthcare, Waukesha, WI). For each of the three diffusion MRI sequences (ssEPI, rFOV and msEPI), 16 axials slices were acquired to cover the entire prostate and reconstructed at a 256$$${\times}$$$256 matrix. Each of the three sequences was acquired in two series with different b-value groups. For ssEPI and rFOV, diffusion images were obtained with low b-values=[10(4 averages), 50(4), 100(4), 200(4), 400(16), 600(16), 800(16)]s/mm$$${^{2}}$$$, and high b-values=[10 (4), 50(4), 100(4), 400(16), 800(16), 1200(16), 1500(16)]s/mm$$${^{2}}$$$, respectively. For msEPI sequence, low b-values=[10(2), 50(2), 100(2), 200(2), 400(8), 600(8), 800(8)]s/mm$$${^{2}}$$$, and high b-values=[10 (2), 50(2), 100(2), 400(8), 800(8), 1200(16), 1500(16)]s/mm$$${^{2}}$$$ were used because of time constraints. Specific parameters used in all sequences are shown in Table 1.
Diffusion estimation: Diffusion parameters were estimated on the averaged signal from regions-of-interest (ROIs) of approximately 0.6cm$$${^{2}}$$$ in the central gland (CG) and 0.8cm$$${^{2}}$$$ in the peripheral zone (PZ) of the prostate for each acquisition. This signal was fitted by non-linear least-square fitting with the following three diffusion models: 1. Mono-exponential model $$S(b)=S_{0}e^{-bADC_m};$$ 2. Stretched exponential model7 $$S(b)=S_{0}e^{-(bD_s)^{\alpha_s}}; $$ 3. Kurtosis model8 $$S(b)=S_{0}e^{-bD_k+\frac{1}{6}b^{2}{D_k}^{2}k}; $$ where $$$S(b)$$$ is the signal intensity for a specific b value, $$$S_0$$$ is the signal intensity at b=0 $$${s/mm^2}$$$. ADC, $$$D_s$$$ and $$$D_k$$$ are the diffusion coefficients for three models respectively. $$$\alpha_s$$$ is the anomalous exponent and $$$k$$$ is kurtosis.
To assess the reproducibility of the diffusion measurements for each of the three signal models, Bland-Altman analysis was performed across different pulse sequences and different b-value groups.
Fig.1 shows representative ssEPI, rFOV and msEPI images, including DW images (b=400s/mm$$$^2$$$), ADC maps obtained from the low b-value acquisition and ADC maps obtained from the high b-value acquisition. Diffusion parameters measured in the CG and PZ using different diffusion models and different pulse sequences are listed in Table 2.
Fig.2 shows Bland-Altman plots of ADC values across different pulse sequences (a) and across b-value groups (b) (remaining Bland-Altman plots not shown for brevity). Table 3 lists the bias with 95$$$\%$$$ confidence interval and p values in Bland-Altman analysis across pulse sequences (a) and across b-value groups (b).
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