Method and magnetic resonance system for imaging a partial region of an examination subject

• US 9,753,113 B2
• Filed: 09/07/2012
• Issued: 09/05/2017
• Est. Priority Date: 09/07/2011
• Status: Active Grant

• Current Assignee: Siemens Healthineers AG (Siemens AG)
• Original Assignee: Siemens AG
• Inventors: Blumhagen, Jan Ole, Fenchel, Matthias, Ladebeck, Ralf
• Primary Examiner(s): Koval, Melissa
• Assistant Examiner(s): Fetzner, Tiffany
• Application Number:
  US13/606,398
• Publication Number:
  US 20130057282A1
• Time in Patent Office: 1,824 Days
• Field of Search: 324300-322, 600407-435
• CPC Class Codes: A61B 5/055 involving electronic [EMR] or nuclear [NMR] magnetic resonance, e.g. magnetic resonance imaging
• CPC Class Codes: G01R 33/481 MR combined with positron emission tomography [PET] or single photon emission computed tomography [SPECT]
• CPC Class Codes: G01R 33/56563 caused by a distortion of the main magnetic field B0, e.g. temporal variation of the magnitude or spatial inhomogeneity of B0 G01R33/56509, G01R33/56518, G01R33/56536 take precedence
• CPC Class Codes: G01R 33/56572 caused by a distortion of a gradient magnetic field, e.g. non-linearity of a gradient magnetic field G01R33/56509, G01R33/56518, G01R33/56536 take precedence

Abstract

In a method and magnetic resonance (MR) apparatus to image a partial region of an examination subject by means of a multislice measurement, which partial region includes at least two measurement slices, and is located at least in part at the edge of a field of view of the magnetic resonance apparatus, for each voxel to be optimized that is located at the edge of the field of view, a gradient field is configured for each measurement slice of the partial region that is to be measured and is used to acquire magnetic resonance data in the multislice measurement. The gradient field is configured so as to cause a nonlinearity of the gradient field and a B₀ field inhomogeneity to cancel at each of the aforementioned voxel to be optimized at the partial region at the edge of the field of view. An image of the partial region of the examination subject is determined from the magnetic resonance data acquired in this manner.

Claims

1. A method to image a partial region of an examination subject in an Imaging system across at least two measurement slices, comprising:

positioning an examination subject in a magnetic resonance data acquisition unit, having a field of view, with a partial region of the examination subject, of which a magnetic resonance image is to be obtained, being located at least in part at an edge of said field of view, said data acquisition unit comprising a gradient coil system and a basic field magnet;

with a computer system, operating said magnetic resonance data acquisition unit with a data acquisition pulse sequence in order to acquire magnetic resonance data of said partial region in a multi-slice measurement in which a slice selection gradient and a readout gradient are activated by the gradient coil system of the data acquisition unit, that respectively produce a slice selection gradient field and a readout gradient field while a basic magnetic field is generated by the basic field magnet of the magnetic resonance data acquisition unit;

operating said magnetic resonance data acquisition unit with said pulse sequence in order to optimize each voxel in said image, that is located at said edge of said field of view, in each of said measurement slices of said partial region, by configuring at least one of said slice selection gradient, or said readout gradient of said pulse sequence, as an at least one configured gradient in said pulse sequence, in order to make a distortion caused by a non-linearity of the respective gradient field of said at least one configured gradient, cancel a distortion caused by a basic magnetic field inhomogeneity of said basic magnetic field that exists at each of said voxels being optimized at said edge of said field of view; and

with said computer system, reconstructing an image of said partial region from said acquired magnetic resonance data.

2. A method as claimed in claim 1 comprising configuring each configured gradient, of said pulse sequence, by:

determining, with said computer system, a relative gradient field error at the respective voxel at the edge of the field of view;

determining, with said computer system, said basic magnetic field inhomogeneity at the respective voxel at the edge of the field of view; and

also

determining, with said computer system, the configured gradient as a result of the determined relative gradient field error and the determined basic magnetic field inhomogeneity at the respective voxel.

3. A method as claimed in claim 2 comprising configuring each gradient field G of each configured gradient field, in the pulse sequence with said computer system according to:

G=−

dB₀(Δ

x,Δ

y,Δ

z)/c(Δ

x,Δ

y,Δ

z)

wherein dB₀ is the basic magnetic field inhomogeneity at the respective voxel (Δ

x,Δ

y,Δ

z) at said edge of said field of view; and

wherein c is the relative gradient field error at the respective voxel Δ

x,Δ

y,Δ

z) at the edge of the field of view.

4. A method as claimed in claim 1 comprising selecting said partial region of said examination subject in order to comprise an anatomical structure of a patient that is located at said edge of said field of view of said magnetic resonance data acquisition unit.

5. A method as claimed in claim 4 comprising selecting said partial region in order to encompass an arm of a human as said examination subject.

6. A method as claimed in claim 1 wherein said magnetic resonance data acquisition unit comprises a tunnel-shaped opening in which said examination subject is located, and wherein said edge of said field of view comprises a sleeve proceeding along an inner surface of said tunnel-shaped opening.

7. A method as claimed in claim 6 wherein said sleeve has a sleeve thickness of 5 cm.

8. A method as claimed in claim 1 comprising operating said magnetic resonance data acquisition unit in order to acquire said magnetic resonance data in a transverse plane with respect to the examination subject.

9. A method as claimed in claim 1, wherein said imaging system further comprises a positron emission tomography data acquisition unit, and comprising, in said computer system, determining an attenuation correction when acquiring positron emission tomography data, dependent on said reconstructed image of said partial region.

10. An imaging apparatus comprising:

a magnetic resonance data acquisition unit having a field of view, a gradient coil system, and a basic field magnet that generates a basic magnetic field;

said magnetic resonance data acquisition unit having a patient opening therein that is configured to receive an examination subject in the magnetic resonance data acquisition unit, with a partial region of the examination subject, of which a magnetic resonance image is to be obtained, being located at least in part at an edge of said field of view;

a processor configured to operate said magnetic resonance data acquisition unit with a data acquisition pulse sequence in order to acquire magnetic resonance data of said partial region in a multi-slice measurement in which a slice selection gradient and a readout gradient are activated in order to cause the gradient coil system of the magnetic resonance data acquisition unit to produce a slice selection gradient field and a readout gradient field, while the basic magnetic field is generated by the basic field magnet of the magnetic resonance data acquisition unit;

said processor being configured to operate said magnetic resonance data acquisition unit with said pulse sequence in order to optimize each voxel in said image, that is located at said edge of said field of view, in each of said measurement slices of said partial region, by configuring at least one of said slice selection gradient, or said readout gradient within said pulse sequence, as an at least one configured gradient in said pulse sequence, in order to make a distortion caused by a non-linearity of the respective gradient field of said at least one configured gradient, cancel a distortion caused by a basic magnetic field inhomogeneity of said basic magnetic field that exists at each of said voxels being optimized at said edge of said field of view; and

an image computer configured to reconstruct a magnetic resonance image of said partial region from said acquired magnetic resonance data.

11. An imaging apparatus as claimed in claim 10 further comprising a positron emission tomography data acquisition unit, and wherein said processor is also configured to determine positron emission tomography data acquisition unit parameters that operate said positron emission tomography data acquisition unit, dependent on said reconstructed magnetic resonance image of said partial region.

12. A non-transitory, computer-readable data storage medium encoded with programming instructions, said data storage medium being loaded into a computerized control and evaluation unit of an imaging apparatus said imaging apparatus comprising:

a magnetic resonance data acquisition unit having a field of view;

a gradient coil system that generates respective gradient fields, each exhibiting a gradient;

a basic field magnet that generates a basic magnetic field; and

an opening configured to receive an examination subject in the magnetic resonance data acquisition unit with a partial region of the examination subject, of which a magnetic resonance image is to be obtained, being located at least in part at an edge of said field of view;

said programming instructions causing said control and evaluation system to;

operate said magnetic resonance data acquisition unit with a data acquisition pulse sequence in order to acquire magnetic resonance data of said partial region in a multi-slice measurement in order to cause a slice selection gradient and a readout gradient to be activated by the gradient coil system of the data acquisition unit that respectively produce a slice selection gradient field and a readout gradient field, while the basic magnetic field is generated by the basic field magnet of the magnetic resonance data acquisition unit;

operate said magnetic resonance data acquisition unit with said pulse sequence in order to optimize each voxel in said image, that is located at said edge of said field of view, by configuring at least one of said slice selection gradient, or said readout gradient within said pulse sequence, as an at least one configured gradient in said pulse sequence, in order to make a distortion caused by a non-linearity of the respective gradient field of said at least one configured gradient, cancel a distortion caused by a basic magnetic field inhomogeneity of a basic magnetic field that exists at each of said voxels being optimized at said edge of said field of view; and

reconstruct a magnetic resonance image of said partial region from said acquired magnetic resonance data.

13. A non-transitory, computer-readable data storage medium as claimed in claim 12 wherein said programming instructions cause said control and evaluation system to determine positron emission tomography data acquisition parameters dependent on said reconstructed magnetic resonance image of said partial region, and subsequently operate a positron emission tomography data acquisition unit of the imaging apparatus with said position data acquisition parameters in order to acquire positron emission tomography data from said partial region.