B1+ correction is essential for quantitative prostate DCE-MRI. A simplified approximated analytical B1+ correction method was proposed previously, and we assess this method on a digital reference object (DRO) with various SNR levels and on 110 in-vivo cases from two 3.0 T systems. We find that the approximated analytical B1+ correction method achieves comparable performance to conventional correction method with substantially reduced computation. The approximated analytical correction method is simple and practical for application in the clinic.
As described previously3, we proposed an approximated analytical B1+ correction method which only takes the B1+ map and uncorrected PK maps as the input. It is easy to implement and can reduce the computation time. The comparison between proposed approximated correction and conventional numerical correction is shown in Fig. 1.
To evaluate our proposed method, we created a prostate-specific digital reference object (DRO) based on the RSNA Quantitative Imaging Biomarkers Alliance (QIBA) project with our clinical protocol4. The DRO comprised of a series of realistic ground truth Ktrans (ranged from 0.01 to 0.35 min-1) and ve (ranged from 0.01 to 0.5). Noise was added to each DRO images using the equation $$$\sqrt{(R+r_1)^2+r_2^2}$$$, which is similar to QIBA DRO v96. R is the original signal, and r1 and r2 are noise with mean zero and standard deviation ranging from 5 to 150. The resulting baseline SNR of the DCE signal is from 7.8 to 234.5. With noise added in all DRO images, B1+ corrected PK maps using two correction methods were calculated for each noise level, and both correction methods were evaluated using mean percentage error compared to the ground truth PK parameters.
With IRB approval, 110 prostate patients acquired from two 3.0T systems (MAGNETOM Skyra and MAGNETOM Trio, Siemens Medical Systems) were retrospectively selected to evaluate the approximated analytical correction by comparing with the conventional numerical correction. For each case, relative flip angle maps were generated based on RR-VFA method7,8, and three Ktrans and ve maps were calculated (uncorrected, approximated analytically corrected, and numerically corrected). Due to data availability, volumetric regions of interest (ROI) of the prostate region were defined for 82 cases, and the lesions on another 28 cases from the same RF system were contoured based on radiology report, as shown in Fig. 2. The approximated analytical correction method was evaluated using percentage error compared to the numerical corrected PK maps. All post-processing was implemented using an in-house script written in Matlab (Mathworks, Inc., Natick, MA, USA). Estimation parameters (Ktrans or ve) larger than 1 were excluded as outliers9.
In the DRO experiment, the correction error with different levels of baseline SNR is shown in Fig. 3. Both correction errors decrease with increased baseline SNR level, and the difference between two correction methods is minimal compared to noise-induced correction error. Also, the numerical correction error has a minimum of 2.1%±4.3% with the maximum SNR of 234.5 in the simulation, which gives the correction uncertainty from noise.
Fig. 4 shows an example in-vivo case with PK maps and error maps. The error induced by the approximation is negligible compared to error induced by B1+ variation. Among the 82 cases, the percentage error of the approximated analytical correction is 0.11±0.27% for Ktrans, and 0.11±0.38% for ve. Fig. 5 shows the B1+ distribution and the approximated analytical correction error for both prostate ROI and lesion ROI. The B1+ patterns between two scanners (Fig. 5a) are significantly different (p < 0.05), indicating the necessity of B1+ correction for comparison between scanners. Similarly, within lesion ROIs, the average B1+ varies from 81.8% to 116.8%, showing the necessity for B1+ correction for lesion characterization. For all the evaluations, the Ktrans and ve errors are less than 0.4%, which is much smaller than the noise-induced uncertainty. Additionally, our proposed correction method computationally took 0.01s for a typical 3D volume cases, while the conventional correction methods took more than 3 hours with our implementation. Our proposed correction method can be a good alternative under some condition regarding computation efficiency.
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