apps.nlinv_maps#
- bartorch.apps.nlinv_maps()#
Coil sensitivity maps fitted to the low-resolution centre of k-space.
One set of maps from
bart nlinv -m 1, normalized to unit root sum of squares over the coils (unit sensitivity for one coil). The maps are fitted on a grid of the low-resolution centre alone, with the Sobolev weighting of the sensitivities scaled to that grid, and zero-filled in k-space to the image grid.- Parameters:
kspace (torch.Tensor) – Complex k-space. Cartesian:
(coils, [z,] y, x)on the reconstruction grid. Non-Cartesian:(coils, shots, samples).traj (torch.Tensor, default=None) – Trajectory
(shots, samples, 3)in units of the image grid;Nonefor Cartesian data. Its kz may be nonzero.size (int, default=24) – Cartesian: lines of every encoded axis, around the centre, the maps are fitted to.
radius (float, default=12.0) – Non-Cartesian: distance from the k-space centre, in grid units, within which samples are fitted, on a grid of
2 ceil(radius)points an axis.shape (tuple of int, default=None) – Non-Cartesian: image grid of the maps,
(y, x)or(z, y, x);Nonefor the one BART estimates fromtraj.phase_pole (int, default=None) – Gauss-Newton step after which the phase poles the maps share are detected and moved into the image (
nlinv --phase-pole); 0 after every step,Nonenever. At a shared phase pole the smoothness of the maps drives every coil’s sensitivity towards zero, and a coil combination over them goes dark there. BART refuses the detection on a grid with an axis no longer than a twentieth of its longest, rounded up: the grid of the central lines, so a volume of fewer than 3 partitions at the defaultsize.
- Returns:
Complex maps: of the shape of
kspacefor Cartesian data,(coils, *shape)otherwise.- Return type:
torch.Tensor
- Raises:
BartError – If
phase_poleis set for a grid too thin for BART’s detection.