Dynamic contrast enhanced magnetic resonance imaging (DCE-MRI) with pharmacokinetic modeling can help to quantify the perfusion and function of liver. The accurate pharmacokinetic modeling relies on the accurately and reliably captured vascular input function (VIF)s. However, due to the fast blood velocity, the blood in the large vessels including abdominal aorta and the main branch of the portal vein experiences only a limited number of excitations and hasn’t reached a steady state. This introduces bias in the VIFs, and consecutively bias in pharmacokinetic parameters. In this study, we sought to correct the inflow effect on VIF acquisition in liver DCE-MRI.
INTRODUCTION
Dynamic contrast enhanced magnetic resonance imaging (DCE-MRI) with pharmacokinetic modeling can help to quantify the perfusion and function of liver which had been applied in malignancy detection, fibrosis stage classification, cirrhosis estimation (1). The accurate pharmacokinetic modeling relies on the accurately and reliably captured vascular input function (VIF)s. However, due to the fast blood velocity, the blood in the large vessels including abdominal aorta and the main branch of the portal vein (PV) experiences only a limited number of excitations and hasn’t reached a steady state. This introduces bias in the VIFs, and consecutively bias in pharmacokinetic parameters. In this study, we sought to correct the inflow effect on VIF acquisition in liver DCE-MRI.THEORY
Considering that the blood in a small branch of the hepatic vein had reached the steady state $$$M_z^{ss}$$$, the equilibrium magnetization $$$M_z^0$$$ can be calculate use the steady state equation $$$M_z^{ss} = \frac{{M_z^0\left( {1 - {e^{ - TR/{T_1}}}} \right)}}{{1 - cos\alpha {e^{ - TR/{T_1}}}}}$$$ with assumed T1. With regard to the blood in a specified location which had not reached the steady state, equation $$$M_z^{\left( n \right)} = M_z^0\left( {1 - {e^{ - TR/{T_1}}}} \right) + M_z^{\left( {n - 1} \right)}cos\alpha {e^{ - TR/{T_1}}}$$$ (2) can be used to calculate the number of excitations ( $$${N_p}$$$ ) the blood had experienced iteratively until $$$M_z^{\left( {{N_p}} \right)}$$$ is equal to the signal intensity measured on the pre-contrast image. Assuming blood velocity is constant, $$${N_p}$$$ of different dynamic phases can be considered as the same to the pre-contrast phase. Thus, with known $$${N_p}$$$ , the changed T1 of blood after contrast can be calculated more accurately using the same equation. Moreover, the flow in the PV can be estimated, since its direction is nearly perpendicular to the axial plane. Therefore, the SPGR-based flow velocity can be estimated as $$${v_{SPGR}} = \frac{D}{{{N_p}TR}}$$$, where $$$D$$$ is the inflow distance, which can be measured from the images.METHODS
In Vivo Experiment and Image Acquisition
After approval of the institutional animal care and use committee, five pigs were scanned at 3.0T (Discovery MR 750, GE Healthcare, Waukesha, WI). The scan protocol include a respiratory navigator triggered dual-echo DISCO (3) for liver DCE acquisition. The imaging parameters for DISCO sequence were TR/TE1/TE2 = 4/1.5/3ms, FA = 12°, slice thickness = 4 mm, axial plane imaging, in-plane resolution = 1.4 mm. The 2D pencil beam navigator was put on the right liver dome, the acceptance window was set to 30% and temporal resolution was about 7s. After the pre-contrast acquisition, 0.25 mmol/kg of contrast agent (Gd-DTPA) was injected through the marginal ear vein at a rate of 2 mL/s followed by 15 mL 0.9% saline solution flush. Moreover, a respiratory triggered 4D flow (PC-VIPR) sequence (4) was acquired as a reference for blood velocity measurements.
Image Analysis
An ROI was put in the right hepatic vein to measure the $$$M_z^{ss}$$$ of blood for the $$$M_z^0$$$ calculation. The T1 value of blood without contrast was assumed as 1500ms (5). ROIs for the arterial (AIF) and portal venous (PIF) input function extraction were selected and the corresponding contrast concentrations were averaged. $$$R1$$$ of Gd-DTPA at 3 Tesla is 5.14 (/mM/s) (6). For the PV, the $$${v_{SPGR}}$$$ was also calculated. ROIs of liver tissue were selected and fitted using Van Beers model (7) with the corrected and uncorrected AIF & PIF, which were compared using a paired t test. The PC-VIPR images were analyzed, and the main PV was selected to derive the flow velocity, $$${v_{PC}}$$$ . Intra-class correlation (ICC) was used to estimate the consistency between $$${v_{PC}}$$$ and $$${v_{SPGR}}$$$ .
RESULTS
Figure 1 showed a reformatted coronal image of the liver before contrast injection. The obvious signal decrease can be seen along the aorta and PV & superior mesenteric vein from the inflow to the outflow direction, which confirms our theory. One example of AIF and PIF before and after correction is displayed in Figure 2. The amplitude of the corrected AIF and PIF were both higher than the uncorrected. The uncorrected AIF&PIF resulted in significantly overestimated perfusion parameters (P = 0.009 for arterial perfusion and P = 0.033 for portal venous perfusion) (Figure 3). Figure 4 shows the estimated pixel-wise $$${v_{SPGR}}$$$ in PV using the proposed method. Figure 5 shows the scatter plot of $$${v_{PC}}$$$ and $$${v_{SPGR}}$$$ . The ICC between $$${v_{PC}}$$$ and $$${v_{SPGR}}$$$ of PV was 0.856.DISCUSSION
This study could prove that a VIF without inflow correction might lead to significant overestimation of flow parameters. The proposed correction method has the potential to correct the inflow related enhancement effect in liver DCE-MRI analysis, and thus might be able to improve the accuracy of kinetic modeling. The agreement of velocity estimation using the proposed method with PC-MRI further validated the feasibility of the method.1. Haider MA, Farhadi FA, Milot L. Hepatic Perfusion Imaging: Concepts and Application. Magnetic Resonance Imaging Clinics of North America 2010;18(3):465-475.
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