J Budde

Human imaging at 9.4 T using T2*-, phase-, and susceptibility-weighted contrast

The effect of susceptibility differences on an MR image is known to increase with field strength. Magnetic field inhomogeneities within the voxels influence the apparent transverse relaxation time T2*, while effects due to different precession frequencies between voxels caused by local field variations are evident in the image phase, and susceptibility‐weighted imaging highlights the veins and deep brain structures. Here, these three contrast mechanisms are examined at a field strength of 9.4 T. The T2* maps generated allow the identification of white matter structures not visible in conventional images. Phase images with in‐plane resolutions down to 130 μm were obtained, showing high gray/white matter contrast and allowing the identification of internal cortical structures. The susceptibility‐weighted images yield excellent visibility of small venous structures and attain an in‐plane resolution of 175 μm. Magn Reson Med, 2011.

Functional MRI in human subjects with gradient‐echo and spin‐echo EPI at 9.4 T

The increased signal‐to‐noise ratio and blood oxygen level dependent signal at ultra‐high field can only help to boost the resolution in functional MRI studies if the spatial specificity of the activation signal is improved. At a field strength of 9.4 T, both gradient‐echo and spin‐echo based echo‐planar imaging were implemented and applied to investigate the specificity of human functional MRI. A finger tapping paradigm was used to acquire functional MRI data with scan parameters similar to standard neuroscientific applications.

Ultra-high resolution imaging of the human brain using acquisition-weighted imaging at 9.4 T

One of the main goals of ultra-high field MRI is to increase the spatial resolution reached in structural and functional images. Here, the possibility to obtain in vivo images of the human brain with voxel volumes below 0.02mm(3) is shown at 9.4T. To optimize SNR and suppress ringing artifacts, an acquisition-weighted 3D gradient-echo sequence is used, which acquires more averages in the center than in the outer regions of k-space. The weighting function is adjusted to avoid losses in spatial resolution and scan duration compared to a conventional experiment with an equal number of scans and otherwise identical parameters. Spatial resolution and SNR of the weighted sequence are compared to conventionally acquired images by means of phantom and in vivo measurements, and show improved image quality with unchanged spatial resolution and an SNR increase of up to 36% in phantoms and 20%±5% in vivo. Ultra-high resolution images with a voxel volume of 0.014mm(3) (0.13×0.13×0.8mm(3)) from the human brain have sufficient SNR and show fine intracortical detail, demonstrating the potential of the technique. The combination of acquisition-weighted imaging and highly sensitive array coils at ultra-high fields thus makes it possible to obtain images with ultra-high spatial resolutions within acceptable scan times.

Design and evaluation of an RF front‐end for 9.4 T human MRI

At the field strength of 9.4 T, the highest field currently available for human MRI, the wavelength of the MR signals is significantly shorter than the size of the examined structures. Even more than at 7 T, constructive and destructive interferences cause strong inhomogeneities of the B1 field produced by a volume coil, causing shading over large parts of the image. Specialized radio frequency hardware and B1 management methods are required to obtain high‐quality images that take full advantage of the high field strength. Here, the design and characteristics of a radio frequency front‐end especially developed for proton imaging at 9.4 T are presented. In addition to a 16‐channel transceiver array coil, capable of volume transmit mode and independent signal reception, it consists of custom built low noise preamplifiers and TR switches. Destructive interference patterns were eliminated, in virtually the entire brain, using a simple in situ radio frequency phase shimming technique. After mapping the B  1+ profile of each transmit channel, a numerical algorithm was used to calculate the appropriate transmit phase offsets needed to obtain a homogeneous excitation field over a user defined region. Between two and three phase settings are necessary to obtain homogeneous images over the entire brain. Magn Reson Med, 2011. &© 2011 Wiley‐Liss, Inc.

Theoretical and experimental evaluation of continuous arterial spin labeling techniques

Continuous arterial spin labeling is known to be the most sensitive arterial spin labeling technique. To avoid magnetization transfer effects and to overcome hardware limitations, several sequences have been proposed that adiabatically label the inflowing blood. Four of these methods are examined with respect to their sensitivity both theoretically by Bloch equation simulations and experimentally. All sequences were optimized carefully by adjusting their measurement parameters based exclusively on the results of simulations. Perfusion measurements on the human brain obtained at 3 T result in excellent images from all techniques, while differences in sensitivity are similar to those expected from the simulations. Magn Reson Med, 2010.

Human brain imaging at 9.4 T using a tunable patch antenna for transmission

For human brain imaging at ultrahigh fields, the traveling wave concept can provide a more uniform B1+ field over a larger field of view with improved patient comfort compared to conventional volume coils. It suffers, however, from limited transmit efficiency and receive sensitivity and is not readily applicable in systems where the radiofrequency shield is too narrow to allow for unattenuated wave propagation. Here, the near field of a capacitively adjustable patch antenna for excitation is combined with a receive‐only array at 9.4 T. The antenna is designed in compact size and placed in close proximity to the subject to improve the transmit efficiency in narrow bores. Experimental and numerical comparisons to conventional microstrip arrays reveal improved B1+ homogeneity and longitudinal coverage, but at the cost of elevated local specific absorption rate. High‐resolution functional and anatomical images demonstrate the use of this setup for in vivo human brain imaging at 9.4 T. Magn Reson Med, 2013.