Magnetic resonance method and apparatus for echo-planar imaging with a zigzag-type trajectory in raw-data space

1. A method for operating a magnetic resonance (MR) apparatus, comprising:

operating an MR data acquisition scanner to execute an echo-planar MR data acquisition sequence in which signal echoes are acquired by applying readout gradients along a readout axis, kx, and phase-encoding gradients along a phase-encoding axis, ky, with said signal echoes being entered asymmetrically into a memory organized as raw-data space yielding a zigzag-type undersampled trajectory such that said signal echoes are shifted in the raw-data space to cause a raw-data center associated with the raw-data space to be offset from a geometric center of the raw-data space with respect to the kx and ky axes, the shift in the raw data space being limited to a maximum of a quarter of the raw-data space in a direction of said readout axis;

in a computer, reconstructing an additional zigzag-type trajectory in the raw-data space by executing a parallel imaging reconstruction algorithm using the zigzag-type trajectory of the acquired signal echoes; and

in said computer, reconstructing at least one MR image from the acquired signal echoes in the raw-data space, using an interlaced Fourier transform and said additional zigzag-type trajectory.

2. A method as claimed in claim 1 comprising, before reconstructing said at least one MR image, extending raw-data points represented by said signal echoes in the raw-data space to form an extension segment, using a point symmetry of the raw-data space with respect to the center of raw-data space, and thereby producing an extended raw-data space comprising said raw-data space and said extension segment, with raw data in said extension segment being calculated using point reflection with respect to said center of the raw-data space.

3. A method as claimed in claim 2 comprising shifting said signal echoes in said direction of said readout axis by a quarter of the raw-data space,

wherein said extension segment is in said direction of the readout axis.

4. A method as claimed in claim 2 , further comprising:

applying said interlaced Fourier transform to said signal echoes in the raw-data space to produce a hybrid space;

applying said interlaced Fourier transform to said extension segment to produce a hybrid extension segment;

merging said hybrid space and said hybrid extension segment to produce a total hybrid space; and

subjecting said total hybrid space to a Fourier transform along said readout axis to produce said at least one MR image.

5. A method as claimed in claim 2 wherein said at least one MR image has a resolution, and wherein a recording time required for acquiring said at least one MR image with said resolution is reduced by not filling the raw-data space completely with raw data that would be necessary for obtaining said resolution, but which corresponds to said extended raw-data space with said extension segment.

6. A method as claimed in claim 2 comprising recording said at least one MR image with a defined recording time, with raw data recorded in said defined recording time, without using said extension segment, being used to reconstruct an MR reference image with a defined resolution, said at least one MR image being reconstructed with said interlaced Fourier transformation using said extension segment so as to give said at least one MR image a higher resolution than said defined resolution.

7. A method as claimed in claim 1 comprising shifting said signal echoes along said readout axis only by an amount that makes a spacing of said zigzag-type undersampled trajectory, relative to the reconstructed additional zigzag-type trajectory, in a direction of the phase-encoding axis of said phase-encoding gradients, smaller than one sampling step in the ky-direction (Δky).

8. A method as claimed in claim 1 comprising reconstructing said additional zigzag-type trajectory using a Generalized Autocalibrating Partially Parallel Acquisition (GRAPPA) reconstruction algorithm.

9. A method as claimed in claim 1 comprising reconstructing said additional zigzag-type trajectory so that an incline of a last segment of said reconstructed zigzag-type trajectory is opposite, in a positive direction of said phase-encoding gradients, to an incline of a last segment of the acquired zigzag-type trajectory.

10. A method as claimed in claim 1 , further comprising:

prior to reconstructing said at least one MR image, extending raw-data points represented by said signal echoes in the raw-data space to form an extension segment; and

shifting said signal echoes in said direction of said readout axis by a quarter of the raw-data space,

wherein said extension segment is in said direction of the readout axis.

11. A method as claimed in claim 1 , further comprising:

prior to reconstructing said at least one MR image, extending raw-data points represented by said signal echoes in the raw-data space to form an extension segment;

applying said interlaced Fourier transform to said signal echoes in the raw-data space to produce a hybrid space; and

applying said interlaced Fourier transform to said extension segment to produce a hybrid extension segment.

12. A method as claimed in claim 11 , further comprising:

merging said hybrid space and said hybrid extension segment to produce a total hybrid space; and

subjecting said total hybrid space to a Fourier transform along said readout axis to produce said at least one MR image.

13. A method as claimed in claim 1 , wherein an average spacing between adjacent points of the raw-data space in a phase-encoding direction satisfies the Nyquist criterion.

14. A magnetic resonance (MR) apparatus comprising:

an MR data acquisition scanner;

a computer configured to operate said MR data acquisition scanner to execute an echo-planar MR data acquisition sequence in which signal echoes are acquired by applying readout gradients along a readout axis, kx, and phase-encoding gradients along a phase-encoding axis, ky, with said signal echoes being entered asymmetrically into a memory organized as raw-data space yielding a zigzag-type undersampled trajectory such that said signal echoes are shifted in the raw-data space to cause a raw-data center associated with the raw-data space to be offset from a geometric center of the raw-data space with respect to the kx and ky axes, the shift in the raw data space being limited to a maximum of a quarter of the raw-data space in a direction of said readout axis;

said computer being configured to reconstruct an additional zigzag-type trajectory in the raw-data space by executing a parallel imaging reconstruction algorithm using the zigzag-type trajectory of the acquired signal echoes; and

said computer being configured to reconstruct at least one MR image from the acquired signal echoes in the raw-data space, using an interlaced Fourier transform and said additional zigzag-type trajectory.

15. A non-transitory, computer-readable data storage medium encoded with programming instructions, said storage medium being loaded into a computer of a magnetic resonance (MR) apparatus comprising an MR data acquisition scanner, and said programming instructions causing said computer to:

operate said MR data acquisition scanner execute an echo-planar MR data acquisition sequence in which signal echoes are acquired by applying readout gradients along a readout axis, kx, and phase-encoding gradients along a phase-encoding axis, ky, with said signal echoes being entered asymmetrically into a memory organized as raw-data space yielding a zigzag-type undersampled trajectory such that said signal echoes are shifted in the raw-data space to cause a raw-data center associated with the raw-data space to be offset from a geometric center of the raw-data space with respect to the kx and ky axes, the shift in the raw data space being limited to a maximum of a quarter of the raw-data space in a direction of said readout axis;

reconstruct an additional zigzag-type trajectory in the raw-data space by executing a parallel imaging reconstruction algorithm using the zigzag-type trajectory of the acquired signal echoes; and

reconstruct at least one MR image from the acquired signal echoes in the raw-data space, using an interlaced Fourier transform and said additional zigzag-type trajectory.