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Diffusion-weighted Echo Planar Spectroscopic Imaging Using semi‐LASER Localization at 3T: A Pilot Study
Manoj Kumar Sarma1,2, Andres Saucedo3, and M. Albert Albert Thomas3
1Advanced Imaging Research Center, UT Southwestern Medical Center, Dallas, TX, United States, 2Radiology, UT Southwestern Medical Center, Dallas, TX, United States, 3Radiology, UCLA School of Medicine, Los Angeles, CA, United States

Synopsis

Diffusion-weighted spectroscopy (DW-MRS) is an excellent tool to explore the compartment specific assessment of tissue microstructure. Although there has been growing interest in DW-MRS for clinical applications, most of the studies involving human brain metabolites so far have used single-voxel methods, which limit its application to specific white matter tracts or arbitrarily selected regions of interest. There has been only a few attempts to evaluate the diffusion properties of brain metabolites with DW-MRSI. Here, we propose an echo planar-based diffusion-weighted spectroscopic imaging using semi-LASER localization and bipolar diffusion gradients. Initial results show good spectral quality and spatial localization.

Introduction:

Diffusion-weighted spectroscopy (DW-MRS) is an excellent tool to explore the diffusion properties of intracellular metabolites1,2 allowing compartment specific assessment of tissue microstructure. Combined with other imaging modalities such as DW-MRI, DW‐MRS has been shown to differentiate between axonal degeneration, glial activation, and demyelination3-5. Although there has been growing interest in DW‐MRS for clinical applications6-9, most of the studies involving human brain metabolite so far used single voxel methods, which limit its application to specific white matter tracts or arbitrarily selected regions of interest. There have been only few attempts to obtain maps of the diffusion properties of brain metabolites with DW-MRSI10-12. One of the reasons for this is the intrinsic low signal-to-noise ratio (SNR) of metabolites, especially at high diffusion-weightings; coupled with signal losses related to B1 field inhomogeneities and chemical shift displacement error. DW-MRS with semi-LASER localization and adiabatic selective refocusing pulses has been shown to minimize these signal losses and a recent study evaluated the feasibility of this method in a clinical setting13. In this study, we develop and evaluate the feasibility of an echo planar-based diffusion-weighted spectroscopic imaging using semi‐LASER localization (DW-sL-EPSI) at 3T, which uses pairs of bipolar diffusion gradients to measure the apparent diffusion coefficient (ADC) of metabolites.

Materials and Methods:

Figure 1 shows the schematic diagram of the DW-sL-EPSI sequence with diffusion sensitizing gradients (DSG) added in a bipolar configuration. A slice‐selective 90° pulse was used for excitation followed by two pairs of slice-selective adiabatic refocusing hyperbolic secant (HS) pulses. Eight bipolar diffusion-weighted gradients where applied around the four HS refocusing pulses in the three orthogonal directions simultaneously with 26.8 ms duration (δ), and 71 ms diffusion time (Δ). The bipolar gradient scheme helps to minimize eddy currents as well as cross terms between the diffusion gradients and gradients rising from inhomogeneities of the B0 field. Spatial-spectral encoding was performed using a series of EPI readout modules. Outer volume suppression and water suppression via WET were implemented using the standard pulse sequence components available.
To examine the efficiency and reliability, brain phantom data were collected using the DW-sL-EPSI on a 3T Prisma MRI scanner equipped with a 16-channel head ‘receive’ coil. Following parameters were used: TE=120 ms, TR=2.5 ms, 1.5x1.5x2 cm3 voxel for VOI localization, 512 bipolar echo pairs, FOV = 16x16 cm2, 12 averages, spectral width 1190 Hz respectively. A non-water-suppressed scan with one average was also recorded for eddy current correction and estimation of coil sensitivities. For both water-suppressed and non-suppressed data, each gradient lobe was applied in 3 orthogonal gradient directions at 2 and 21 mT/m resulting in b = 36 and 3996 s/mm2. A non-zero b-value for the low b acquisition was used to assist suppressing unwanted echo pathways. The signal processing of DW-sL-EPSI data and spectral quantification based on peak integral was performed using a custom MATLAB (the Mathworks, Inc., Natick, MA) program. Metabolite and water ADCs were estimated from mono-exponential fits.

Results and Discussion:

Figure 2(A) shows the T1-weighted localization image with VOI represented by a solid rectangle. Figure 2(B) and (C) shows the spectra obtained from the 3x3 voxel within the VOI. Even at high b-value of 3996 s/mm2, the quality of the MR spectra was sufficient to quantify the metabolites. There was no noticeable difference in the metabolite line shape, and the quality of the spectrum was sufficiently restored. Typical ADC maps for Glx (Glutamate + Glutamine) from a phantom measurement is shown in Figure 3(a). Metabolite ADC map was roughly homogeneous showing less variation in ADC estimation inside the VOI. Table 1 shows ADC values for – four metabolites, total N-Acetylaspartate (tNAA), total choline (tCho), creatine (Cr) and Glx – calculated from the DW-EPSI phantom experiments which ensured the accuracy of the DW-sL-EPSI results. The ADC values were consistent with previous studies6,10,14. This demonstrates feasibility of implementing DW-sL-EPSI with bipolar DSG and semi-LASER localization at 3T. As DSGs are applied only in a single direction, the present work does not provide rotationally invariant estimates of ADCs. Still, the DW-sL-EPSI results are in agreement with previous studies. One of the limitations of the current implementation is the long scan time that could limit clinical investigations. This can be overcome using accelerated imaging technique such as non-uniform sampling combined with compressed sensing and machine learning15,16.

Conclusion:

Combining semi-LASER localization, echo planar readout and bipolar DSG, we have demonstrated the pilot feasibility of DW-sL-EPSI. While these initial results are promising, further optimization and validation with a large pool of human subjects is needed. Future work will address robust sampling and acceleration techniques.

Acknowledgements

This research was supported by grants from 1) NIH/NHLBBI (5R01HL135562-03), and 2) a Breakthrough Step I grant from the US Congressionally Directed Medical Research Program (CDMRP)/ Breast Cancer Research Program (BCRP) (W81XWH-16-1-0524).

References

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Figures

Figure 1: Schematic representation of the DW-sL-EPSI sequence showing RF pulses with bipolar DW gradients placed around the slice selective refocusing HS RF pulses. δ = gradient duration, sum of the durations of four lobes; Δ = diffusion time, time between the first lobe of the dephasing diffusion gradient group and the first lobe of the re-phasing diffusion gradient group. Water suppression was performed with WET. An EPI-based readout was used to capture the k-t data.

Figure 2: Results from a brain phantom scan. (A) T1-weighted localization image showing the VOI; also shown is the DW-sL-EPSI spectra obtained from the 3x3 region within the VOI at the b-values (B) 36 s/mm2 and (C) 3996 s/mm2.

Figure 3: (A) Metabolite ADC maps for Glx overlaid on the T1-weighted localization image of a phantom measurement; extracted spectra from the central voxel at (9, 9) for the two b-values, (B) 36 s/mm2 (low) and (C) 3996 s/mm2 (high). The spectra were scaled with respect to the NAA peak at 1.9 ppm for the low b-value.

Table 1: Estimated metabolite ADC (×10-3 mm2/s) value over the 4x4 voxels inside the VOI.

Proc. Intl. Soc. Mag. Reson. Med. 29 (2021)
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