The inhomogeneous (ihMT) technique represents a relatively simple addition to MT, but provides a different contrast that is sensitive to the dipolar relaxation time T1D. A review is provided of: method(s) for its application; considerations for optimizing the ihMT signal; the use of models to obtain quantitative parameters and guide acquisition; and its application in vivo.
The relatively novel inhomogeneous MT (ihMT) technique has sparked interest based on demonstrations of greater signal in myelin containing tissues, as found in the central nervous system (CNS) (Fig. 1), and close to zero signal from other tissue types1,2. The method is based on the difference in the signal following RF irradiation at a single offset frequency Δf, and the signal from a dual frequency (±Δf) saturation preparation, achieved by cosine modulation or alternating frequency RF pulses (Fig. 2). The potential contribution from MT asymmetry, due to use of data acquired following RF saturation applied at varying offset frequencies, has been studied at ultra-high field3. As for MT, it is possible to optimize the ihMT signal based on the RF saturation scheme4, and can be applied in various means to 2D/3D MRI sequences alike1,2,5.
The nomenclature stems from initial thoughts that the differences in saturation are due to inhomogeneous broadening underlying the short T2 line associated with the macromolecular, bound component. In particular, the differential saturation was thought to be more specific to the lipid membranes6,7, found in high concentration in myelin of the CNS, which itself forms a major part of white matter. Greater understanding of the mechanism, including use of a dipolar reservoir in MT models, shows ihMT to be sensitive to the dipolar relaxation time, T1D8 and the result of inhomogeneous saturation behavior of dipolar broadened lines. Single offset frequency saturation effectively couples the Zeeman pool with the dipolar reservoir (assuming a non-zero T1D), thus limiting the efficiency of the saturation. On the other hand, dual-offset irradiation decouples the Zeeman pool from the dipolar order, which gives a more efficient saturation9,10 (Fig. 2a). The larger ihMT signal in the CNS, and lamellar liquid crystalline samples, is associated with spin systems with residual dipolar couplings and relatively long T1D (>3ms), which is itself found to be temperature dependent11. IhMT signal in short T1D tissues, e.g. muscle, are found to be weak but still measurable. The potential sensitivity to white matter and grey matter tissues is improved by optimization of the RF pulses utilized12, and greatly enhanced by low duty RF power deposition13,14 (Fig. 3).
The ihMT technique has been compared with diffusion tensor imaging in healthy spinal cords and shows variation with cervical level, age, and between white matter fascicles15. To date, application of ihMT in studies of: amyotrophic lateral sclerosis16, cervical spondylotic myelopathy17, multiple sclerosis18,19, and a mouse model for experimental autoimmune encephalomyelitis20, has shown ihMT to be a useful complimentary MRI technique. In most cases any changes detected were more significant relative to regular MT.
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