Method and system for creating magnetic resonance images

1. A method for creating magnetic resonance (MR) images of a target object, the method comprising:

performing, using a MR system, a respective reference scan of the target object, for each slice of the target object to be imaged, to record a reference dataset, the performance of each of the respective reference scans including separately performing a Gradient Echo (GRE) sequence or a Rapid Acquisition with Refocused Echoes (RARE) sequence for each of the respective slices of the target object to be imaged;

performing, using the MR system, a respective phase correction scan of the target object, for each slice of the target object to be imaged, to record a correction dataset, the performance of each of the phase correction scans including performing a non-phase-encoding Echo-Planar Imaging (EPI) sequence for each of the slices of the target object to be imaged;

performing, using the MR system, a Simultaneous Multislice (SMS) sequence to record a measurement dataset of the target object;

determining slice-specific Generalized Autocalibrating Partial Parallel Acquisition (GRAPPA) kernels based on the reference dataset; and

creating, by a processor of the MR system, the MR images of the target object based on the measurement dataset using a slice GRAPPA method, wherein creating the MR images includes:

separating data of the measurement dataset belonging to different slices of the slices imaged from one another based on the slice-specific GRAPPA kernels; and

correcting Nyquist-N/2 ghost artifacts in the measurement dataset based on the correction dataset.

2. The method as claimed in claim 1 , wherein the reference scans for all slices are carried out one after the other and the phase correction scans for all slices are carried out one after the other, all of the phase correction scans being carried out after all of the reference scans have been carried out.

3. The method as claimed in claim 1 , wherein the reference scans for all slices are carried out one after the other and the phase correction scans for all slices are carried out one after the other, all of the phase correction scans being carried out before all the reference scans are carried out.

4. The method as claimed in claim 1 , wherein:

the reference scans and the phase correction scans are carried out in a nested order; and

for each of the slices to be imaged, the respective reference scan and the respective phase correction scan are carried out before the respective reference scans and phase correction scans for a next slice of the slices to be imaged.

5. The method as claimed in claim 4 , wherein only one excitation pulse is created for each one of the slices, and after the excitation pulse, the respective reference scan and the respective phase correction scan are carried out for the respective slice, without a second excitation pulse being created for the respective slice between the respective reference scan and the respective phase correction scan for the respective slice.

6. The method as claimed in claim 1 , wherein each of the phase correction scans comprises at least three echoes to record the correction dataset, an average value being formed from a first of the at least three echoes and a third echo of the at least three echoes to obtain a temporal consistency with a respective second echo of the at least three echoes.

7. The method as claimed in claim 1 , wherein flip angles of less than 90° are used for the reference scans and the phase correction scans.

8. The method as claimed in claim 1 , wherein the measurement dataset is recorded using a multiband simultaneous multislice Echo-Planar Imaging (SMS-EPI) sequence to provide a diffusion-based imaging of the target object.

9. The method as claimed in claim 1 , wherein the reference dataset is recorded with a lower resolution than the measurement dataset.

10. The method as claimed in claim 1 , further comprising determining sensitivity variations between different receiver coils, of the MR system, used in parallel for the recording of the measurement dataset, wherein the MR images of the target object are created using the determined sensitivity variations.

11. The method as claimed in claim 1 , wherein creating the MR images additionally uses an in-plane GRAPPA method, the method further comprising calibrating the GRAPPA kernels for the in-plane GRAPPA method based on the reference dataset.

12. A non-transitory computer-readable storage medium with an executable computer program stored thereon, that when executed, instructs a processor to perform the method of claim 1 .

13. A magnetic resonance (MR) system, comprising:

a MR scanner configured to record MR data for a target object; and

a data processor configured to process the recorded MR data, the data processor including a memory that stores a computer program, and a processor communicatively coupled to the memory and configured to execute the computer program to:

control the MR scanner to perform a reference scan of the target object to record a reference dataset, the performance of the reference scan including separately performing a Gradient Echo (GRE) sequence or a Rapid Acquisition with Refocused Echoes (RARE) sequence for each respective slice of the target object to be imaged;

control the MR scanner to perform a phase correction scan of the target object to record a correction dataset, the performance of the phase correction scan including performing a non-phase-encoding Echo-Planar Imaging (EPI) sequence for each slice of the target object to be imaged;

perform a Simultaneous Multislice (SMS) sequence to record a measurement dataset of the target object;

determine slice-specific Generalized Autocalibrating Partial Parallel Acquisition (GRAPPA) kernels based on the reference dataset; and

create MR images of the target object based on the measurement dataset using a slice GRAPPA method, wherein creating the MR images includes:

separating data of the measurement dataset belonging to different slices of the slices imaged from one another based on the slice-specific GRAPPA kernels; and

correcting Nyquist-N/2 ghost artifacts in the measurement dataset based on the correction dataset.

14. The method as claimed in claim 1 , wherein for each of the respective slices: only a single excitation pulse is created, and the respective reference scan and the respective phase correction scan are carried out after the single excitation pulse.