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Dissolved 129Xe images were acquired using a 3D radial sequence that employed a pseudo-random view ordering [23], [24] and that selectively excited HP 129Xe with a 1.2-ms, 3-lobe sinc pulse applied at a frequency 3826 Hz higher than the gas phase 129Xe resonance.
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Linear sequences exhibited significantly greater values of Emax than radial sequences (P = .001).001
However, radial sequences were observed to produce a wider spread in Tmax and frequently enhanced at later time points than the equivalent linear sequences.
However, radial sequences reached peak enhancement at a later time than linear sequences at FAs of both 14° (P = .025) and 18° (P < .0001).0001
Those curves derived from radial sequences were found to be relatively insensitive to initial CA uptake and possessed reduced amplitude in comparison with their linear counterparts.
There were no significant differences in the failure rate of fat suppression between linear and radial sequences on statistical analysis of the Rad/Lin-14 and Rad/Lin-18 groups (n = 29, P = .264).264
A self-gated radial VIBE sequence [2] and PET Listmode data were acquired.
First, the radial GRE Sequence can be used to modifying the data acquisition in order to minimize the motion effects.
The 3D radial GRE sequence can provide excellent motion-controlled images with high spatial resolution in noncooperative patients, especially sedated children, at the expense of a longer acquisition time (approximately 2-3 minutes) [ 12].
The 3D radial KWIC sequence may be able to provide useful motion-insensitive data for dynamic MR imaging, that is, time-resolved subframe images, with reasonably high temporal (approximately 3 5 seconds) and spatial resolution [ 15, 19– 219.
On the radial PDW-sequence, the site and extent of labral tears and focal cartilage lesions was found.
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