3D centre-out Yarn-Ball k-space acquisition is implemented in a wind-out/wind-in dual-echo format for the first time. As with standard 3D-Radial acquisition this technique facilitates short (first ‘echo’) TE with utility for imaging tissues with short T2*. However, the advantage of centre-out Yarn-Ball is much greater k-space sampling efficiency than 3D-Radial. Smooth variation from wind-out to wind-in minimizes potential errors in k-space trajectory evolution as a result of eddy-currents. Spoiled-steady-state dual-echo 3D Yarn-Ball images with 0.7x0.7x0.7 mm3 voxels were acquired from the knee of a healthy volunteer in 6 minutes, and the difference image shows ligament and meniscus conspicuity.
Perhaps the first approach one might consider in the implementation of dual-echo Yarn-Ball is simply to replay the gradient waveform backwards (i.e. staring from the end) with inverted polarity (Figure 1). In theory this will resample k-space in reverse (i.e. toward the middle) along the same path. However, sharp transitions within the waveform can lead to ‘unexpected’ k-space sampling delays and deviation from the intended path as the result of eddy-currents. An alternative approach is to continue the direction of winding, rather than reverse it as in Figure 1. A key aspect of the Yarn-Ball technique is that radial evolution (r′) decreases with distance from the centre of k-space as r′=c/r2. At the edge of the sampled k-space sphere (i.e. kmax) typical Yarn-Ball trajectories will be travelling near perpendicular to the radial dimension (i.e. r′ will be very small). Thus, a switch to solving r′=-c/r2 to wind back in will result in minimal radial discontinuity. To ensure sufficient r′ reduction at the point of radial direction change, the trajectory can be solved slightly past kmax with increased radial slowing. While winding out, the azimuthal and polar angles evolve as θ′=cr′ and φ′=crθ′ respectively. To maintain the same winding direction θ′=c|r′| is solved on the way back in.
Images were acquired from a healthy 19 year old female volunteer on a Siemens Prisma 3T scanner using a 4-channel flexible receive-coil wrapped around the knee. The k-space sampling readout duration (or time from the centre of k-space to kmax and visa-versa on return) was chosen to be 2 ms for this initial test. Longer readouts will result in increased signal smearing from rapid T2* decay, but will yield greater sampling efficiency within peripheral nerve stimulation constraints. Slab select excitation along the superior-inferior dimension resulted in a TE of 0.22 ms for the first image; a TE of 5.1 was chosen for the second image. The inclusion of gradient spoiling resulted in a TR of 6.5 ms and a flip-angle of 6o was chosen to maximize signal. A pictorial description of the sequence is given in Figure 2. A total of 18445 trajectories fully sampled k-space for 130 mm isotropic FoV support with 0.7x0.7x0.7 mm3 voxel volume (defined by 1/2kmax). The acquisition of 3 averages yielded a total scan time of 6 minutes. Images were created with standard gridding reconstruction.
[1] Du J., et. al., Magn Reson Imaging, 29(4):470–482, 2011
[2] Stobbe R.W. and Beaulieu C., ISMRM, abstract 2442, 2015 (Toronto)
[3] Martirosian, P., et. al., Magn Reson Med, 71:294–301, 2014