Cardiac Diffusion
Martijn Froeling1

1Radiology, UMC Utrecht, Utrecht, Netherlands

Synopsis

In this talk will review the current standing of diffusion imaging and modeling in the heart. With appropriate data quality and processing diffusion weighted imaging and modeling allows to describe both the microstructural properties of heart tissue as well as describe and quantify its macroscopic anatomy.

Highlights

  1. Challenges in cardiac diffusion weighted imaging are low SNR, image deformations, motion, and perfusion. Being aware of these issues is essential for clinical use of cardiac diffusion imaging.
  2. Measuring diffusion in the presence of motion is challenging. However with the correct sequence design reliable signal can be obtained even in the beating heart.
  3. Applications of diffusion imaging in the heart is twofold: characterizing microstructure and describing macroscopic architecture.

Problem Summary

For clinical applications of diffusion weighted imaging (DWI) in the heart it is important to understand the influence of artifacts, data quality and other confounding factors. Acquiring DWI data that can be used for diffusion tensor imaging (DTI) has been shown feasible over two decades ago. However, DWI in the heart has specific challenges in acquisition an processing that need to be addressed for successful use in a clinical setting. In this talk I will first review the current standing of diffusion imaging and modeling and it pitfalls and limitations. Next I will give an overview of the sequences that can be used for in-vivo cardiac diffusion imaging (1) and demonstrate the models used to describe cardiac microstructure and architecture.

Cardiac Diffusion

DWI of the can be challenging due to its low T2 relaxation time of only 30 to 50 ms. DWI imaging is typically done using a spin echo - echo planar imaging sequence (SE-EPI) . To allow for ample diffusion weighting echo times are generally between 80 and 110 ms, which results in very low SNR. Luckily, the diffusion of water in the heart is fast (MD ≈ 1.6 to 1.8 mm2/s) so a b-value between 400 and 500 s/mm2 is optimal for DTI analysis. The diffusion in the heart fast, this also means that the diffusion anisotropy is much lower (FA ≈ 0.20 to 0.25) and much more sensitive to noise (2, 3). For accurate estimation of diffusion tensor parameters an SNR of 25 of higher is needed (40 or higher for tractography). Investigating microstructural changes in the heart using DWI is mostly done using the DTI model. However, other models are being explored, e.g. IVIM and DKI.

DWI of the beating heart is challenging due to that the heart is always moving. Measuring the microscopic motion of water in the presence of macroscopic motion needs a different diffusion sequence design. To overcome this two different approaches are possible:

1) using a stimulated echo acquisition (STEAM) which applies the diffusion (4) weighting over two consecutive heartbeats and

2) Designing the diffusion weighting wave form to become insensitive for macroscopic motion (5).

With STEAM acquisition it is essential that both diffusion gradients are applied in the identical location of two subsequent cardiac cycles. Typically this is done in the so called “sweet spots” to prevent strain encoding of the diffusion signal (6, 7). Due to improvements in gradient hardware single shot SE sequence with motion compensated gradient wave forms is feasible (8, 9). Due to the long mixing time in STEAM the FA is higher than in SE acquisition. Furthermore the MD is lower in STEAM than in SE acquisition (8). Both methods provide similar data quality however SE has higher scan time efficiency.

Diffusion tensor imaging in the heart is of great interest since it allows to, next to diffusion parameters, obtain detailed information about the cardiac myocardial architecture. The heart has a unique structure with myocytes aligned in a left-handed helix in the epicardium, to circumferential in the mid wall, to a right handed-helix in the endocardium. The heart muscle fibers are arranged in a laminar structure, called sheetlets. Both these structures can be described by quantitative values derived from the diffusion tensor Eigen-vectors. Changes in the myocardial helix angels over the cardiac cycle (10) during development (11) and in pathology (12) have been studied and can potentially give new insights in cardiac function and disease and monitory of cardiac therapy (13).

Acknowledgements

No acknowledgement found.

References

1. Froeling M, Strijkers GJ, Nederveen AJ, Chamuleau SA, Luijten PR: Diffusion Tensor MRI of the Heart - In Vivo Imaging of Myocardial Fiber Architecture. Curr Cardiovasc Imaging Rep 2014; 7:1–11.

2. Damon BM: Effects of image noise in muscle diffusion tensor (DT)-MRI assessed using numerical simulations. Magn Reson Med 2008; 60:934–944.

3. Froeling M, Nederveen AJ, Nicolay K, Strijkers GJ: DTI of human skeletal muscle: The effects of diffusion encoding parameters, signal-to-noise ratio and T2 on tensor indices and fiber tracts. NMR Biomed 2013; 26:1339–1352.

4. Nielles-Vallespin S, Mekkaoui C, Gatehouse P, et al.: In vivo diffusion tensor MRI of the human heart: Reproducibility of breath-hold and navigator-based approaches. Magn Reson Med 2013; 70:454–465.

5. Stoeck CT, Von Deuster C, GeneT M, Atkinson D, Kozerke S: Second-order motion-compensated spin echo diffusion tensor imaging of the human heart. Magn Reson Med 2016; 75:1669–1676.

6. Tseng WYI, Reese TG, Weisskoff RM, Wedeen VJ: Cardiac diffusion tensor MRI in vivo without strain correction. Magn Reson Med 1999; 42:393–403.

7. Dou J, Tseng WYI, Reese TG, Wedeen VJ: Combined diffusion and strain MRI reveals structure and function of human myocardial laminar sheets in vivo. Magn Reson Med 2003; 50:107–113.

8. von Deuster C, Stoeck CT, Genet M, Atkinson D, Kozerke S: Spin echo versus stimulated echo diffusion tensor imaging of the in vivo human heart. Magn Reson Med 2015; 0:n/a-n/a.

9. Aliotta E, Wu HH, Ennis DB: Convex optimized diffusion encoding (CODE) gradient waveforms for minimum echo time and bulk motion-compensated diffusion-weighted MRI. Magn Reson Med 2016; 0:1–13.

10. McGill LA, Scott AD, Ferreira PF, et al.: Heterogeneity of fractional anisotropy and mean diffusivity measurements by in vivo diffusion tensor imaging in normal human hearts. PLoS One 2015; 10:e0132360.

11. Mekkaoui C, Porayette P, Jackowski MP, et al.: Diffusion MRI Tractography of the Developing Human Fetal Heart. PLoS One 2013; 8:e72795.

12. McGill L-A, Ismail TF, Nielles-Vallespin S, et al.: Reproducibility of in-vivo diffusion tensor cardiovascular magnetic resonance in hypertrophic cardiomyopathy. J Cardiovasc Magn Reson 2012; 14:86.

13. Mekkaoui C, Reese TG, Jackowski MP, Bhat H, Sosnovik DE: Diffusion MRI in the heart. NMR Biomed 2015(August).

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