Pulsed magnetization transfer (MT) imaging has been applied to quantitatively assess brain pathology in several diseases, especially multiple sclerosis (MS). To date, however, because of the high power deposition associated with the use of short, rapidly repeating MT prepulses, clinical application has been limited to lower field strengths. The contrast-to-noise ratio (CNR) of MT is limited, and this method would greatly benefit from the use of higher magnetic fields and phased-array coil reception. However, power deposition is proportional to the square of the magnetic field and scales with coil size, and MT experiments are already close to the SAR limit at 1.5T even when smaller transmit coils are used instead of the body coil. Here we show that these seemingly great obstacles can be ameliorated by the increased T 1 of tissue water at higher field, which allows for longer maintenance of sufficiently high saturation levels while using a reduced duty cycle. This enables a fast (5-6 min) high-resolution (1.5 mm isotropic) whole-brain Magnetization transfer ratio (MTR) imaging (1-5) has been used as a noninvasive method to quantitatively assay white matter (WM) degeneration in multiple sclerosis (MS) (4,6 -14) and more recently in neuropsychiatric diseases such as Alzheimer's disease and bipolar disorder (15)(16)(17). Since MT imaging is exquisitely sensitive to the solid-like macromolecular content of central nervous system (CNS) tissue, it can detect subtle pathological changes and sometimes even conventionally unobserved pathology (18,19). Pulsed MT imaging (1,20) employs a series of short (ϳ10 -30 ms), high-amplitude pulses, and relies on the build-up of a saturation steady state over multiple TR periods (1) as opposed to the large saturation induced by continuous wave (CW) experiments within a single TR. The increased speed provided by pulsed MT has allowed investigators to survey the frequency dependence of the MT effect and to determine MT-based parameters, such as fractional pool sizes and exchange rates, within a reasonable clinical scan time (4,10 -12,21-23). However, this comes at the price of a reduced contrast-to-noise ratio (CNR) and increased power deposition, which comes close to maximum specific absorption rate (SAR) levels, even when the transmit/receive head coil is used at a field strength of 1.5T. To harness the power of parallel imaging (24) and further reduce the scan time, it is necessary to use a larger coil (i.e., a body coil in standard sensitivity encoding (SENSE) imaging) for transmission, which unfortunately exacerbates the power-deposition problem. This SAR restriction also appears to be a prohibitive barrier for translating pulsed MT to higher field strengths (e.g., 3T), where a higher signal-to-noise ratio (SNR) would allow faster scan times or an improved contrast-to-noise ratio.
MT acquisition with excellent anatomical visualization of gray matter (GM) and white matter (WM) structures, and even substructures. The method is demonstrated in nine normal volunteers and five patients...