Liver IVIM MR imaging: improved reproducibility of pseudo-diffusion coefficient D* via proper signal modeling
Shih-Han Hung1, Meng-Chieh Liao1, Cheng-Ping Chien1, Wen-Chau Wu2, and Hsiao-Wen Chung3

1Graduate Institute of Biomedical Electronics and Bioinformatics, National Taiwan University, Taipei, Taiwan, 2Graduate Institute of Oncology, National Taiwan University, Taipei, Taiwan, 3Electrical Engineering, National Taiwan University, Taipei, Taiwan

Synopsis

A new scheme was proposed to analyze intravoxel ihcoherent motion MR imaging data of the liver. The method integrated the combined use of single- and bi-exponential signal decaying models to deal with regions with absence of prominent vasculature, and the removal of data obtained at b-values less than 15s/mm2 to avoid contamination from large vessels. Results from ten healthy subjects scanned twice at 3T showed substantially improved reproducibility in the pseudo-diffusion coefficient D*, while those of the true diffusion coefficient and the profusion fraction were unaltered. Using our scheme the estimated D* mostly fall within 38 to 85x10-3 mm2/s.

Introduction

Intravoxel incoherent motion (IVIM) MR imaging has been emerging as a potentially plausible technique that can quantitatively assess both water molecular diffusion and capillary blood perfusion noninvasively in human liver 1. To date, however, the numerical values reported for the pseudo-diffusion coefficient that reflects liver perfusion, D*, vary to a great extent from 27 to 190mm2/s 2-4. It is hypothesized that modeling of the signal decaying behavior plays a role in D* quantification, in addition to effects of respiratory motion 5. In this study, therefore, we aim to increase the reproducibility of D* measurements via proper selection of the signal decaying model and the b-values. Results on 10 healthy subjects scanned twice showed substantial improvements in inter-scan reproducibility in D*.

Theory

Derivation of liver D* using IVIM imaging is based on fitting of the signals as a function of b-values using the bi-exponential decaying model: Sb = S0 [ f*e-bD* + (1-f)*e-bD ], where Sb and S0 are the signal intensities at a specific b value and b=0, respectively, D the true diffusion coefficient, and f the fraction of blood flow in the region of interest (ROI). At least two problems could cause fitting uncertainty. First, in the absence of prominent vasculature, single exponential model suffices, and over-fitting may result when using bi-exponential model. Second, the presence of large vessels may dominate the data at b-values less than 15s/mm2, leading to D* over-estimation 6. To solve these issues, we first restricted curve fitting using data with b>15s/mm2, followed by the combined use of single- and bi-exponential models for fitting, for which the one exhibiting smaller residual fitting error was chosen for the region of interest.

Materials and Methods

All experiments, IRB approved, were carried out on a Siemens 3T scanner with a torso array for signal receiving. Image data at sixteen b-values (0, 10, 20, 30, 40, 50, 60, 70, 80, 90, 100, 150, 200, 400, 600 and 800 s/mm2) were obtained from ten healthy young subjects using respiratory-triggered spin-echo EPI with diffusion sensitizing gradients. Each subject was scanned twice on the same day with re-positioning to examine inter-scan reproducibility. Scanning parameters were: FOV=310x310 or 410x410mm, TE/TR=75/2000ms, thickness=7mm, matrix size=112x112, NEX=6. For estimations of IVIM parameters, circular ROIs at about 1cm diameter were placed on the right hepatic lobe (Fig.1). Curve fitting to derive D* was performed using the proposed scheme described above, with the consistency between two measurements of the identical subjects analyzed using the Bland-Altman plot, and compared with conventional fitting results using solely the bi-exponential model. All data processing was carried out with self-designed Matlab scripts.

Results

Figures 2 and 3 show the Bland-Altman plots for D and D*, respectively. The proposed scheme yielded similar level of reproducibility around 19% imprecision (Fig.2a) to that using the conventional bi-exponential model for the true diffusion coefficient D (Fig.2b) and for the perfusion fraction f (not shown). On the other hand, D* reproducibility was improved substantially from 104% imprecision using conventional bi-exponential model (Fig.3a) to 39% imprecision using the proposed scheme (Fig.3b). With our method, D* for the ten subjects mostly fall within the range of 38 to 85x10-3 mm2/s.

Discussions and Conclusion

Prominent inconsistency in the numerical values for liver D* has been found in past reports employing IVIM imaging 2-4, 6. Results from our study suggest that such phenomena may have originated, at least in part, from inappropriate use of the signal model for curve fitting. Our proposed scheme yielded substantially improved inter-scan D* reproducibility on repeated scans, while precisions in D and f were unaltered. The method may find potential in clinical evaluation of liver perfusion using IVIM MR imaging.

Acknowledgements

No acknowledgement found.

References

1. Koh et al., AJR 2011;196:1351.

2. Andreou A et al., Eur Radiol 2013;23:428.

3. Wurnig MC et al., MRM 2015;74:1414

4. Kakite S et al. JMRI 2015;41:149.

5. Lee Y et al., Radiol 2015;274:405.

6. Cercueil JP et al., Eur Radiol 2015;25:1541.

Figures

Figure 1. Axial diffusion-weighted images (b= 0 and 200s/mm2) showing the selection of regions of interest for analysis.

Figure 2. Bland-Altman plots for diffusion coefficient D using conventional bi-exponential decaying model (a) and the proposed scheme (b). Similar imprecision levels of about 19% were found for both.

Figure 3. Bland-Altman plots for pseudo-diffusion coefficient D* estimated using conventional bi-exponential decaying model (a) and the proposed scheme (b). The proposed method was shown to substantially improve the imprecision (104%) as compared with 39% using the conventional bi-exponential model.



Proc. Intl. Soc. Mag. Reson. Med. 24 (2016)
2947