Quantitative Myocardial Perfusion
Hui Xue1, Michael S Hansen1, and Peter Kellman1

1National Heart Lung and Blood Institute, National Institutes of Health, Bethesda, MD, United States

Synopsis

Quantification of myocardial blood flow (MBF, in the unit of ml/min/g) is more objective to assess myocardial micro-circulation under rest and pharmaceutical or exercise stress condition and capture global flow reduction. Although perfusion quantification has been studies for the past 20 years, it is still not clear how to build a practical quantitative myocardial perfusion workflow. This syllabus reviews key components of such system and emphasizes on motion correction, intensity to Gd concentration conversion and Gd kinetics modelling. With recent developments more focusing on the automation and completeness of entire workflow, including fully automated processing and motion correction, the quantitative perfusion is becoming clinically practical.

Introduction

Myocardial perfusion magnetic resonance imaging has been established as a high sensitive, non-invasive, non-toxic imaging technique with superior spatial resolution to evaluate the myocardial blood flow, compared to the nuclear imaging such as SPECT or PET or more invasive coronary catheterization [1]. The majority of MR perfusion imaging is conducted with cardiac triggering and relies on continuously measuring the myocardium signal during the passage of T1 shortening contrast agent gadopentetate dimeglumine (Gd-DTPA) over sufficient number of heart beats (e.g. 40-60) [2]. The perfusion images are usually evaluated by visual assessment and semi-quantitative metrics, e.g. upslope of time intensity curves. Compared to these methods, quantification of myocardial blood flow (MBF, in the unit of ml/min/g) is more objective to assess myocardial micro-circulation under rest and pharmaceutical or exercise stress condition and quantify absolute flow reduction. It also has the potential to be superior in differentiating global blood flow reduction, such as multi-vessel diseases or micro-vascular diseases.

Accuracy of perfusion flow quantification highly depends on the correct measurement of arterial input function (AIF). Since longer saturation time leads to saturated signal intensities in perfusion imaging during the contrast uptake, either “dual-bolus” [3] or “dual-sequence” [4] technique has been proposed for more accurate AIF estimation. The former relies on injecting a very low dose bolus and assumes the signal linearity between contrast concentration and signal intensity. The latter modified the saturation recovery sequence to acquire a low resolution image (so-called AIF images) with very short saturation time; therefore the signal saturation is less severe. Compared to the "dual-bolus" method, the “dual- sequence” technique requires only one contrast injection and simplifies the clinical workflow. The assumption of signal linearity to Gd concentration can be removed by converting the signal intensity of AIF and perfusion images to Gd concentration unit ([Gd], mmol/L).

As a nontrivial step, the Gd concentration signals of AIF and perfusion images are inputted into certain contrast kinetics model for the estimation of MBF and other parameters. These parameters characterize myocardial microvascular structures, such as blood volume (ml/g) or plasma volume (ml/g), interstitial volume (ml/g) and extraction fraction E .

Since the complete imaging of contrast uptake will take ~60 or more heart beats, it is not possible to breath-hold patients. The breath-holding should not be used during perfusion imaging; but this requires to develop effective motion correction (MOCO) to correct respiratory motion. As shown in Figure 1, a complete workflow of quantitative perfusion imaging includes image acquisition, motion correction on AIF and perfusion series, intensity to [Gd] conversion and Gd kinetics modelling. This syllabus will overview the entire workflow for quantitative myocardial perfusion process.

Imaging sequence

Saturation recovery (SR) based perfusion imaging sequence is the current 'standard' for myocardial perfusion imaging. The advantage of SR in perfusion imaging is its less sensitive to heart rate variation and more myocardial coverage with multiple slices, given a good saturation can be achieved over the heart. It is necessary to use composite RF pulses for SR to have good B0 and B1 insensitivity or to use B1-insensitive pulses (e.g. BIR-4). To correct surface coil inhomogeneity, it is often to acquire proton density weighted (PD) images before the SR readouts. The low resolution AIF imaging module can be inserted after the R-wave to get AIF signal. Figure 2 gives an illustration of SR based perfusion imaging sequences. More detailed review can be found at [2] and [5].

Motion correction

The purpose of MOCO is to restore the correct spatial alignment of myocardium during contrast passage. This step is essential for the free-breathing acquisition. Considerable amount of effort had been made to develop robust, fully automated MOCO solution for perfusion imaging [6–8]. Majority of algorithms utilize the non-rigid image registration to estimate spatial movement and deformation among perfusion images taken at different heart beats. The main difficulties of this task lie on the rapid and drastic contrast changes in perfusion images. Figure 3 illustrates an example of perfusion MOCO. To enable perfusion quantification, it is necessary to correction motion among AIF series. Also, co-registration of PD images to perfusion images is a required feature.

Intensity to [Gd] conversion

Often, perfusion quantification relies on certain assumption that contrast concentration is linearly proportional to image intensity [9,10]. This assumption is very hard to hold, given the variation of dosage, infusion rate, and imperfect imaging sequences and image reconstruction. For the "dual-sequence" scheme, the AIF imaging module has very different parameters (e.g. spatial resolution, readout types). It is impossible to simply take image intensity and assume they represent the [Gd] values correctly. Moreover, perfusion imaging readout can be SSFP for better SNR and AIF readout may remain FLASH. In this case, intensity values cannot be compared directly. The assumption of signal linearity to Gd concentration can be completely removed by converting the signal intensity of AIF and perfusion images to Gd concentration unit ([Gd], mmol/L). This strategy was previously proposed with FLASH perfusion imaging sequences [11,12] and extended to work in SSFP readout [13], as shown in Figure 4.

Gd kinetics modelling

The AIF and perfusion signal has been converted into [Gd] unit with the signal nonlinearity corrected. They serve as inputs to the flow mapping. The principle to estimate MBF from [Gd] concentration utilizes the dynamics of Gd transport across the capillary membrane from the vascular space to the interstitial space. An in-depth review of this topic can be found at [14]. The Gd kinetics models can be divided into two categories: compartmental and distributed parameter (DP) models. In the category of compartmental model, the Fermi function [15] or BSpline based model free deconvolution [16] or exponential decay [17] had be applied to myocardial perfusion. As well illustrated in prior publications [14,17–25], the assumption behind these models is the Gd delivery to the myocardial interstitial space from vascular space is flow limited, at least at the low flow scenario. Thus, the compartmental models do not explicitly count for the Gd extraction from the vascular space into the interstitial space. More studies [26–28] have suggested the Gd delivery to the myocardium is not necessarily flow limited, especially under the stress condition. Since the compartmental model assumes spatially invariant distribution or instantaneous mixing of Gd concentration [14,17] and does not explicitly estimate the influence of extraction fraction (0≤E≤1, a dimensionless scalar, the fraction of Gd extracted from vascular space into the interstitial space [29]), more comprehensive distributed parameter models are applied to the estimate of myocardial blood flow in MRI [14,26–28,30] and in PET [31–33]. Besides the estimation of myocardial blood flow (ml/min/g), distributed models [26–28] were studies to estimate other parameters characterizing myocardial microvascular structures, including blood volume (ml/g) or plasma volume (ml/g), interstitial volume (ml/g) and extraction fraction E .

Other aspects

There are more advanced imaging sequences for perfusion imaging, e.g. 3D k-t sampling [34] and spiral perfusion imaging [35]. To compute MBF from these sequences, two difficulties are motion correction and [Gd] conversion.

The DP models can estimate more parameters, besides MBF, to characterize microvascular structure of myocardium. The potential of those parameters is of strong interests for microvascular diseases and non-ischemic cardiovascular diseases.

The validation of MBF is not an easy task. Animal validation on MBF estimates has been performed against the microsphere in dog or canine models [3,16,20,36,37]. In-vivo validation compared MR MBF values to PET imaging [31,32,38]. A more recent approach is to compare perfusion flow to coronary sinus flow estimation [39].

Fully automated myocardial quantitative perfusion solution has been developed and integrated on the clinical MR scanners [13]. This package includes optimized SR perfusion sequences, motion correction, intensity to [Gd] conversion, different Gd kinetics models. The motion corrected perfusion images and pixel-wise MBF maps are sent to the scanner without any user interaction. Figure 5 gives examples of pixel-wise MBF maps generated with this automated inline quantitative perfusion package.

Conclusions

Quantitative myocardial perfusion has been studies for the past 20 years. With recent developments more focusing on the automation and completeness of entire workflow, including fully automated processing and motion correction, the quantitative perfusion is becoming clinically practical.

Acknowledgements

No acknowledgement found.

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Figures

Figure 1. Overview of the workflow of quantitative perfusion flow mapping. After raw kspace data are reconstructed, resulting AIF and perfusion images go through the motion correction step, which allows the free-breathing acquisition. The AIF LV blood pool is automatically detected from the MOCO AIF series. Both AIF signal and normalized MOCO perfusion images are converted into [Gd] unit by look-up-table conversion. AIF Gd curve and perfusion Gd images are inputted into Gd kinetics models for pixel-wise myocardial flow mapping.

Figure 2. Schematic illustration of SR perfusion imaging sequence. After each SR pulse train, the AIF and perfusion images are read out with certain TD time. Proton density images are acquired first without playing out the SR pulses. The AIF readout can acquire two echoes to estimate T2* signal loss caused by contrast uptake. The table lists some typical imaging parameters used in 1.5T and 3T.

Figure 3. MOCO is to remove the respiratory motion in the perfusion series and restore the spatial alignment of myocardial pixels.

Figure 4. Scheme to convert image intensities to Gd concentration. The key step is to compute a look-up table with the expected [Gd] on one axis and normalized intensity SR/PD on the other axis. Given the sequence parameters used in the perfusion imaging, Bloch simulation can be performed to compute expected magnetization magnitude of PD and SR images. The ratio of these two magnetization is the normalized signal intensity.

Figure 5. Examples of perfusion myocardial flow maps. Patients with normal perfusion (a) have globally well preserved MBF. Patients with single (b) and triple vessel diseases (c) have reduced flow in one or more coronary sectors. The pixel-wise MBF map also cover and go beyond myocardial infarction zone (d).

Proc. Intl. Soc. Mag. Reson. Med. 25 (2017)