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. 2013 May;69(5):1217-25.
doi: 10.1002/mrm.24357. Epub 2012 Jun 12.

Spin-echo magnetic resonance spectroscopic imaging at 7 T with frequency-modulated refocusing pulses

Affiliations

Spin-echo magnetic resonance spectroscopic imaging at 7 T with frequency-modulated refocusing pulses

He Zhu et al. Magn Reson Med. 2013 May.

Abstract

Two approaches to high-resolution SENSE-encoded magnetic resonance spectroscopic imaging (MRSI) of the human brain at 7 Tesla (T) with whole-slice coverage are described. Both sequences use high-bandwidth radiofrequency pulses to reduce chemical shift displacement artifacts, SENSE-encoding to reduce scan time, and dual-band water and lipid suppression optimized for 7 T. Simultaneous B0 and transmit B1 mapping was also used for both sequences to optimize field homogeneity using high-order shimming and determine optimum radiofrequency transmit level, respectively. One sequence ("Hahn-MRSI") used reduced flip angle (90°) refocusing pulses for lower radiofrequency power deposition, while the other sequence used adiabatic fast passage refocusing pulses for improved sensitivity and reduced signal dependence on the transmit-B1 level. In four normal subjects, adiabatic fast passage-MRSI showed a signal-to-noise ratio improvement of 3.2±0.5 compared to Hahn-MRSI at the same spatial resolution, pulse repetition time, echo time, and SENSE-acceleration factor. An interleaved two-slice Hahn-MRSI sequence is also demonstrated to be experimentally feasible.

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Figures

Figure 1
Figure 1
Pulse sequences developed for slice-selective MRSI at 7T. (A) Hahn-MRSI (90°-90°), (B) AFP-MRSI (90°-180°-180°) sequences. In both cases, signal excitation is preceded by (C) a dual-band water and lipid suppression with integrated outer-volume suppression (OVS).
Figure 2
Figure 2
Theoretical signal dependence of the 90°-90° (B1×sin(α)×sin2(α/2)) and 90°-AFP (B1×sin(α)) sequences as a function of the transmit B1 field relative to a nominal B1 field corresponding to a 90° rotation. Off-resonance effects and the effects of relaxation are ignored in these simulations. For comparison, the B1 dependence of a conventional 90°-180° spin echo sequence (B1×sin3(α)) is also shown.
Figure 3
Figure 3
Metabolic images recorded using the AFP-MRSI sequence in one subject. In addition to the sagittal (showing MRSI slice location) and axial anatomical MR images, the transmit B1 map, and reconstructed metabolic images of images of glutamate and glutamine (Glx), myo-inositol (mI), choline (Cho), creatine (Cr) and N-acetyl aspartate (NAA) normalized to the H2O-MRSI are shown. Histograms of the transmit B1 distribution and the frequency (B0) distribution after high order shimming in this slice location are also shown. 59% of MRSI voxels fell within the range +/− 10 Hz.
Figure 4
Figure 4
AFP-MRSI spectra from the whole slice of the dataset as shown in Figure 3.
Figure 5
Figure 5
Comparison of spectra using the Hahn-MRSI and AFP-MRSI pulse sequences in the same voxel (left parietal gray matter) from one subject; top trace is the original spectra and baseline fit, middle trace the baseline-subtracted experimental data overlaid with the results of the fitting routine, and the bottom trace the residual. The approximately 3-fold greater SNR of the AFP-MRSI sequence under the same acquisition conditions is apparent. However, the SAR of the AFP-MRSI sequence was more than double that of the Hahn-MRSI sequence (53% vs. 24%, respectively). Mild residual lipid (Lip) contamination is present.
Figure 6
Figure 6
Hahn-MRSI spectra from one slice of the 2-slice dataset recorded in one subject. In these experiments, note the incomplete lipid unfolding upfield from the NAA peak in central voxels, due to errors in the SENSE-reconstruction algorithm used.

References

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