The two dimensional J-resolved spectroscopy technique is capable of resolving many metabolites in vivo from a volume of interest. However, the spectral resolution along the indirect dimension is generally very poor in these acquisitions. One solution is to apply a covariance transformation along the indirect dimension to yield a resulting Covariance J-resolved (CovJ) spectrum with high spectral resolution. While spectral resolution is enhanced, currently there are no methods available to fit the non-linear aspects of the covariance reconstruction. Here, we have developed a non-linear fitting algorithm capable of yielding Glutamate, Glutamine, GABA, and Glutathione concentrations in vivo using CovJ spectra.
Processing: From a JPRESS experiment4, an acquired data set is stored as a 2D matrix, $$$a(t_2,t_1)$$$, where $$$t_2$$$ and $$$t_1$$$ are the directly and indirectly sampled temporal dimensions, respectively. JPRESS data were processed as previously discussed3. CovJ spectra were produced by applying the covariance transformation in the mixed spectral-temporal domain, $$$\widetilde{A}(F_2,t_1)$$$, where $$$F_2$$$ is the direct spectral domain. The resulting CovJ spectrum, $$$S$$$, can be found using5: $$S = [Re(\widetilde{A}) \cdot Re(\widetilde{A}^T)]^{\frac{1}{2}} + [Im(\widetilde{A}) \cdot Im(\widetilde{A}^T)]^{\frac{1}{2}}$$ $$$Re(\widetilde{A})$$$ and $$$Im(\widetilde{A})$$$ are the real and imaginary parts of $$$\widetilde{A}$$$, respectively. $$$S$$$ is a square matrix and the indirect CovJ spectral dimension, $$$F_1’$$$, has the same spectral bandwidth and spectral resolution as $$$F_2$$$.
Cov-SEHAR algorithm: A diagram explaining the fitting process can be seen in Figure 1. Corrections are applied to the acquired data using ProFit 2.0 preprocessing for phasing and frequency drifts6,7. First, the algorithm fits the concentrations and line-broadening of the JPRESS singlet resonances of N-acetyl aspartate (NAA), Creatine 3.0 (Cr3.0), and Phosphocholine (PCh). The second fit uses these values and a specific part of the CovJ spectrum, the 2.15 – 2.65ppm region, to evaluate Glu, Gln, GABA, and GSH. Since the cross-peaks are most interesting for this evaluation, the diagonal signals are nulled using a spectral mask. The second fit also assigns each metabolite a damping factor, or $$$T_2$$$* value, along the $$$t_1$$$ dimension. The objective functions in Figure 1 are minimized by using a built-in, non-linear MATLAB solver, lsqnonlin. Finally, scaling factors accounting for proton numbers are utilized to give Glu, Gln, GABA, and GSH values with respect to the total signal in that area (Glu+Gln+GABA+GSH).
Simulations: Maximum-echo sampled4 J-resolved prior-knowledge for NAA, Cr3.0, PCh, Glu, Gln, GABA, and GSH were simulated using the GAMMA library8. These were simulated with TE = 30ms, direct spectral bandwidth = 2000Hz, indirect spectral bandwidth = 1000Hz, and $$$(t_2,t_1)$$$ points = (2048,100). These metabolites were scaled to typical in vivo concentrations for gray matter9. In addition, Glu+Gln (Glx) was added with varying Gln/Glx percentages to produce 4 unique spectra with 0%, 15%, 30%, and 45% Gln/Glx concentrations.
In Vivo Acquisitions: A total of 24 healthy volunteers (mean age = 65 years old) were consented and scanned on a Siemens 3T Trio scanner (Siemens Healthcare, Erlangen, Germany). The scan parameters are listed above, and the voxel was placed on the medial frontal gray matter for all volunteers using a voxel size of 2.5x2.5x2.5cm$$$^3$$$ and a TR=2500ms. All subjects were evaluated using Cov-SEHAR and statistical analysis was performed to yield mean, standard deviation, and correlation to Glu values for all metabolites.
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