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Optimized PRESS Echo Time for Quantifying Relative ω-3 Fat Content at 9.4T In Vivo
Clara J. Fallone1, Anthony G. Tessier 1,2, Catherine J. Field3, and Atiyah Yahya1,2
1Department of Oncology, University of Alberta, Edmonton, AB, Canada, 2Department of Medical Physics, Cross Cancer Institute, Edmonton, AB, Canada, 3Department of Agricultural, Food, and Nutritional Science, University of Alberta, Edmonton, AB, Canada

Synopsis

Omega-3 (ω-3) fat content in adipose tissue is relevant to the study of disease. It is challenging to quantify with Magnetic Resonance Spectroscopy (MRS) due to its low concentration in vivo. In addition, its resonance is difficult to resolve from that of the non-ω-3 protons, even at 9.4T. A PRESS (Point RESolved Spectroscopy) echo time of 109ms was determined to yield resolved ω-3 (≈ 0.98ppm) and non-ω-3 (≈ 0.9ppm) methyl peaks at 9.4T. The efficacy of the sequence was verified on oil phantoms and on rats fed a high ω-3 fat diet.

Introduction

Omega-3 (ω-3) dietary fat intake correlates inversely with disease, including obesity 1, bone disease 2,3, and breast cancer 4, and is reflected in adipose tissue fat composition 5-8. Magnetic Resonance Spectroscopy (MRS) can assess fat composition in vivo 9-16; however, ω-3 fat quantification is challenging due to low abundance of ω-3 fats (≈ 1%) in adipose tissue 17. Omega-3 fats have their first carbon-to-carbon double bond on the third carbon from the end-chain fatty acid methyl. Consequently, the ω-3 methyl protons (≈ 0.98ppm) have a higher chemical shift than the non-ω-3 methyl protons (≈ 0.9ppm) and neighbor the allylic (≈ 2.1ppm) protons, whereas the non-ω-3 methyl protons neighbor the methylene (1.3ppm) protons 18,19. Figure 1 illustrates the distinction between ω-3 and non-ω-3 fats. At field strengths of 1.5T and 3T, MRS methods based on a long echo time (TE) 19, J-difference editing 20 and the methyl linewidth 21 have been investigated for quantifying ω-3. Higher magnetic field strengths are commonly employed to study animal models. The better spectral resolution enables separately quantifying saturated, mono-unsaturated and di-unsaturated fatty acids 22,23. Negligible levels of ω-3 fatty acids 22,23 are often assumed because of the low concentration of ω-3 fats 17 and because the ω-3 methyl resonance overlaps the non-ω-3 resonance with standard short-TE techniques. Studies show that ω-3 levels are altered in disease 24,25, correlate with bone health 26, and change with diet 5-8; therefore, enabling ω-3 measurement at higher fields is valuable. Recently, a study at 7T utilized PRESS with an ultra-long TE (1000ms) to resolve the ω-3 methyl peak from the non ω-3 methyl and the methylene resonances 27. The objective of this work is to determine an optimal PRESS echo time (<< 1000ms to reduce T2 losses) to quantify relative ω-3 fat content at 9.4T, another commonly employed high field strength for animal studies.

Methods

The response of the methyl resonances to a spin echo sequence was calculated using product operator formalism 20,28. The ω-3 and non-ω-3 methyl protons were modeled as A2X systems, with X as one of three methyl protons and A1 and A2 as the neighboring allylic protons (for ω-3 fats) or methylene protons (for non-ω-3 fats) 20. The term leading to methyl proton observable magnetization is $$X_{x}[\frac{1}{2}+\frac{cos(2\pi JTE)}{2}]$$ where J denotes the coupling constant between the methyl and methylene protons. The methyl protons form a triplet signal, with a constant central peak $$$[\frac{X_{x}}{2}]$$$ and sinusoidal side multiplets $$$[\frac{X_{x}cos(2\pi JTE)}{2}]$$$. Timings where the side multiplets of the ω-3 and non-ω-3 methyl triplets are 0 minimize overlap between the two peaks and occur for TE values of $$$[\frac{2n+1}{4J}]$$$, where n is an integer. Assuming a coupling constant of 6.9Hz 29 yields a TE of 109ms when n = 1. All experiments were conducted with a 21cm diameter 9.4T animal magnet. PRESS spectra were acquired from 5x5x5mm3 voxels from five spherical oil phantoms with varying ω-3 fat content (0% to 57%, determined using 16.5T NMR), using a volume coil. Spectra were acquired with TE values of 25ms (TE1 = 15ms, TE2 = 10ms) and 109ms (TE1 = 15ms, TE2 = 94ms). The sequence efficacy was verified in vivo on a rat fed a high ω-3 fat diet for 12 weeks. The diet consisted of 20% weight/weight fat. The fat portion was 16% ω-3, comprising of 20% flax oil, 30% lard, 40% olive oil, and 10% DHA (docosahexanoic acid). Gated PRESS spectra were obtained from the rat with short and long TE from a 5x5x5mm3 voxel in the visceral fat of the rat abdomen using a rat volume coil (Doty Scientific). The ω-3 to non-ω-3 peak area ratio was calculated for the oils and the rat.

Results

Figure 2 displays spectra obtained from the oils at 9.4T using the short and optimized long TEs. Figure 3 indicates the linear correlation (R2 = 0.9974) between the actual ω-3 to non-ω-3 fat ratio of the oils (determined from 16.5T NMR) and the relative peak area ratio measured using PRESS (TE = 109ms) at 9.4T. Figure 4 displays spectra acquired from the rat using short and long TE values from the voxel shown. The ratio of ω-3 methyl to non ω-3 methyl peak areas in the rat was 0.13 using PRESS with TE of 109ms and the ω-3 methyl peak SNR was 65.

Discussion

PRESS with a total TE of 109ms resolves the ω-3 methyl resonance from that of non-ω-3 at 9.4T in phantoms and in rat adipose tissue in vivo. The improved spectral resolution at 9.4T enabled using a shorter TE value than 1000ms, which was employed at 7T 27 to minimize contamination from methylene protons, reducing T2 losses. The optimal TE provides a coefficient of determination of 0.9974 for relative measures of ω-3 to non- ω-3 content; T2 and J-coupling losses prevent absolute quantification. The TE of 109ms was calculated to obtain 0 signal for the side multiplets for methyl resonances. In the experimental spectra some multiplet signal is visible, likely due to evolution of anti-phase coherences during signal detection 28.

Conclusion

PRESS with TE of 109ms resolves the ω-3 methyl peak from the non ω-3 methyl peak at 9.4T in vivo.

Acknowledgements

Grant and student funding from the Natural Sciences and Engineering Research Council of Canada is gratefully acknowledged.

References

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Figures

Figure 1: A non-ω-3 poly-unsaturated fatty acid (linoleic acid, top), and an ω-3 fatty acid (linolenic acid, bottom). The ω-3 molecule is characterized by the carbon-to-carbon double bond that occurs on the third carbon from the end-chain methyl group. Consequently, the ω-3 methyl protons neighbor the ≈ 2.1ppm allylic protons and resonate at ≈ 0.98ppm. In comparison, the non-ω-3 methyl protons neighbor the 1.3ppm methylene protons and resonate at ≈ 0.9ppm.

Figure 2: Spectra acquired from five oils of varying ω-3 content using PRESS with short TE (25ms) and optimized long TE (109ms) at 9.4T. Using the long echo time, the ω-3 methyl peak can be resolved from the non-ω-3 methyl peak.

Figure 3: Linear correlation between the actual ω-3 to non-ω-3 fat content of the oils (calculated from 16.5 T NMR) and the peak area ratio measured using PRESS with TE of 109ms at 9.4T.

Figure 4: Spectra acquired from the rat abdomen using PRESS with short TE (25ms) and optimized long TE (109ms). Using the long echo time, the ω-3 methyl peak can be resolved from the non-ω-3 methyl peak. The PRESS voxel (5x5x5mm3) location is shown on axial and coronal images.

Proc. Intl. Soc. Mag. Reson. Med. 28 (2020)
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