0106

Improved Quantification of Ktrans with Cardiac Output Based Correction of Arterial Input Function
Artem Mikheev1, Louisa Bokacheva1, Jeff Lei Zhang2, Hersh Chandarana1, Sungheon Gene Kim3, and Henry Rusinek1
1Department of Radiology, New York University School of Medicine, New York, NY, United States, 2School of Biomedical Engineering, ShanghaiTech University, Shanghai, China, 3Department of Radiology, Weill Cornell Medical College, New York, NY, United States

Synopsis

The arterial signal in DCE MRI often suffers from the inflow effect, which may cause large errors in the arterial concentration and compartmental model analysis. We implemented a constrained signal-to-concentration conversion using the subject’s cardiac output based on the Stewart-Hamilton principle, which limits the area under the arterial first pass peak. The constrained conversion significantly reduced the variation of the arterial concentration sampled at three levels along the abdominal aorta. The constrained arterial input function resulted in a significantly lower variability of the Tofts model Ktrans in psoas muscle compared to the uncorrected input function.

Introduction

Reliable estimates of the arterial input function (AIF) are critical to the model analyses of dynamic contrast-enhanced (DCE) MRI. However, the blood signal is often affected by various factors, such as the RF coil sensitivity, hematocrit, and inflow artifact, which may cause large errors in model parameters1. We implemented a method to compute the AIF concentration constrained by the subject’s cardiac output (CO). The method forces the area under the AIF’s first pass to obey the Stewart-Hamilton principle of indicator dilution2. Here we evaluate the effectiveness of the constrained conversion to reduce the variability of Ktrans due to the variations of the AIF sampled at different levels along the abdominal aorta.

Methods

This retrospective study was approved by the institutional review board. Subjects were selected from an existing dataset of renal DCE MRI exams (N=116) acquired with the same protocol3. One female and one male subject were selected to represent each of 7 decades by age (20-29 years old, 30-39,…, 80-89 years old) for a total of 14 exams (7 women and 7 men; age, mean±stdev, 55±21 years; age range, 24-87 years). DCE MRI was acquired at 1.5 T (MAGNETOM Avanto, Siemens Healthcare, Erlangen, Germany) for at least 6 min after an injection of 4 mL Gd-DTPA using 3D FLASH (TR=2.84 ms; TE=1.05 ms; FA=12°; matrix, 256x256x40; voxel, 1.66x1.66x2.5 mm3; temporal resolution, 3 s during 0-40 s post-injection and 15-60 s afterwards).

Image analysis was performed in FireVoxel, a freely available research software package (NYU School of Medicine, firevoxel.org). Using fully automatic image derived input function (IDIF)4, we generated, for each subject’s abdominal aorta, three signal curves Si,j(t), where i=1,…,14 is the subject number and j=1,2,3 is the sampling location: (1) 3 cm superior to the renal arteries (RA), (2) at RA; (3) 3 cm inferior to RA.

Constrained signal-to-concentration conversion was implemented in FireVoxel (Fig. 1). The bolus arrival time (BAT) and recirculation time (RCT, the transition between the first pass peak and the recirculation peak) were identified automatically. These time points were used to find the baseline signal S0i,j and the area under the first pass peak, which was determined from the gamma variate fit5. The aortic signal curves Si,j(t) were first converted to concentration Ci,j(t) using regular conversion based on spoiled gradient echo signal equation and fast water exchange limit6 with T10=1480 ms for blood7 and contrast agent relaxivity8 r1=4.25 (mM s)-1. For each subject, the cardiac output (COi) was estimated as COi = CI x BSAi, where the cardiac index CI was assumed to be fixed at 2.7 L/min/m2 for all subjects9 and BSAi was the subject’s body surface area10. The CO-constrained concentration curves C’i,j(t) were computed by iterative fitting.

Regions of interest (ROIs) (24.2±12.1 cm3) were drawn over each subject’s psoas muscle. The ROI-averaged signal was converted to concentration with T10=1100 ms for muscle11. Muscle concentration was fitted with the two-parameter Tofts model12. Model fitting was performed with the original, unconstrained Ci,j(t) and then with constrained C’i,j(t) as the AIF, yielding Ktransi,j and Ktransi,j, respectively. The variation of Ktrans due to the AIF sampling level was estimated as Di = (|Ktransi,1 – Ktransi,2| + |Ktransi,2 – Ktransi,3| + |Ktransi,3 – Ktransi,1|)/3 and similarly as D’i with Ktrans’i,j.

The AIF variability due to sampling level was estimated as Ei = (P’i – Pi)/Pi, where Pi = (‖Ci,1(t) – Ci,2(t)‖ + ‖Ci,2(t) – Ci,3(t)‖ + ‖Ci,3(t) – Ci,1(t)‖)/Ci,avg and Ci,avg was each subject’s mean arterial concentration averaged across the three levels (Ci,1(t), Ci,2(t), Ci,3(t)) between BAT and the last time point. The post-correction P’ was defined similarly, with C’i,j replacing Ci,j. The correlation of the AIF difference with age was assessed using Pearson coefficient. The comparison of Pi and Pi’, Ktransi and Ktransi’ and Di and D’i, was done using one-tailed, paired t-test, assuming p=0.05 to indicate significance.

Results

The mean Ktrans was 0.107±0.090 mL/min/mL with regular conversion and 0.045±0.027 mL/min/mL with constrained conversion (p=0.005) (Fig. 2A). The variation of Ktrans was significantly reduced after constrained conversion (p=0.006) (Fig. 2B). The estimated CO (mean±stdev) was 5.4±0.7 L/min (women, 5.1±0.5 L/min; men, 5.7±0.8 L/min). The mean AIF differences decreased by 57%±20% (p<0.001) after constrained conversion (Fig. 3). The AIF variations tended to be larger in younger subjects with regular conversion (p=0.06), but this trend disappeared after constrained conversion. The differences of the aortic signal baseline with sampling level, which led to large variations of the concentration curves obtained with regular conversion, decreased after constrained conversion (Fig. 4).

Discussion

The constrained conversion reduced both the mean values and the differences in Ktrans due to the variations of the AIF with the sampling location. The post-correction Ktrans values were in agreement with the values obtained in psoas muscle13 and in leg muscles14 using commercial software employing a population-based AIF. Here, we determined Ktrans using the subjects' own AIFs and individualized CO estimates. The resulting distribution of CO was in good agreement with published values15. The correction was less effective in a case with motion artifacts (Fig. 2B). The constrained conversion is expected to improve Ktrans quantification in well-perfused tissues, as well as in younger subjects with stronger inflow effect.

Acknowledgements

NIH/NIBIB U24 EB02898

References

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Figures

Figure 1: The CO-based constrained conversion algorithm diagram.

Figure 2: A. The mean Ktrans values in each subject due to the AIF variation with sampling level decreased significantly after constrained conversion (regular, 0.107±0.090 mL/min/mL; constrained, 0.045±0.027 mL/min/mL, p=0.005). B: The mean difference in each subject among Ktrans (mL/min/mL) due to the AIF variation with sampling level decreased significantly after constrained conversion (regular, 0.055±0.061; constrained, 0.009±0.017; p=0.006).


Figure 3: Normalized AIF difference over sampling levels in each subject decreased significantly after constrained conversion (mean±stdev: regular, 1.51±0.73; constrained, 0.60±0.35; p<0.001).


Figure 4: A. DCE MRI images of a 28-y.o. subject. Left: Coronal slice through the abdominal aorta (left) at maximum aortic enhancement, with AIF sampling locations. Center: Psoas muscle at maximum aortic enhancement; right: the same slice at maximum muscle enhancement. B. Signal-time curves at three levels. C. Concentration-time curves with regular conversion showing large differences. D. Concentration-time curves with constrained conversion showing smaller differences.

Proc. Intl. Soc. Mag. Reson. Med. 30 (2022)
0106
DOI: https://doi.org/10.58530/2022/0106