Method and magnetic resonance apparatus for non-selective excitation of nuclear spin signals in an examination subject

Patent metadata

Field	Value
Publication number	US-9523755-B2
Application number	US-201213630232-A
Country	US
Kind code	B2
Filing date	Sep 28, 2012
Priority date	Sep 30, 2011
Publication date	Dec 20, 2016
Grant date	Dec 20, 2016

Abstract

In a method for non-selective excitation of nuclear spin signals in an examination subject with a magnetic resonance system, RF excitation pulses are radiated to excite nuclear spin signals in the examination subject with simultaneous switching of gradients for spatial coding of the excited nuclear spin signals, wherein the RF excitation pulses are designed such that the base frequency of a radiated RF excitation pulse is adapted to the simultaneously switched gradient. By the dynamic adaptation of the radiated RF excitation pulses to the respective simultaneously switched gradients, artifacts due to insufficiently excited nuclear spins in an examination region to be examined (in particular even in examination regions that are arranged off-center) are avoided.

First claim

I claim as my invention:

1. A method for non-selective excitation of nuclear spin signals in an examination subject in a magnetic resonance (MR) apparatus, comprising:
placing an examination subject in an MR data acquisition unit and exposing the examination subject to a basic magnetic field in the MR data acquisition unit;
from a computerized control unit, controlling a scan of the examination subject to acquire MR data therefrom by generating and providing a pulse sequence to the MR data acquisition unit that operates the MR data acquisition unit, with the examination subject therein, to radiate a plurality of non-selective radio-frequency (RF) excitation pulses into the examination subject that each has a base frequency that non-selectively excites nuclear spins in the examination subject and thereby produces MR signals resulting from the excited nuclear spins, while simultaneously activating a phase coding magnetic field gradient that spatially encodes the MR signals, and thereby producing a combined magnetic field in said MR data acquisition unit that is a superimposition of said basic magnetic field and said phase coding magnetic field gradient, said combined magnetic field changing during said scan due to the switching of the phase coding magnetic field gradient; and
in said computerized control unit, automatically setting the base frequency of each non-selective RF excitation pulse in said pulse sequence dependent on the combined magnetic field that exists at a time in said pulse sequence at which that respective non-selective RF pulse is radiated, due to the phase coding magnetic field gradient that is simultaneously switched at said time.

2. The method as claimed in claim 1 wherein said examination subject comprises an examination region in which said nuclear spins are excited and from which said magnetic resonance signals emanate, said examination region exhibiting a Larmor frequency that results from said combined magnetic field, and comprising, in said computerized control unit, automatically setting said base frequency of the non-selective RF excitation pulse to said Larmor frequency that results from said combined magnetic field.

3. The method as claimed in claim 1 wherein said RF excitation pulse has a phase, and comprising, in said computerized control unit, also automatically setting said phase of said non-selective RF excitation pulse dependent on said simultaneously switched phase coding magnetic field gradient.

4. The method as claimed in claim 1 wherein said MR data acquisition unit comprises a measurement volume having a center, and comprising radiating said non-selective RF excitation pulse having said adapted base frequency into an examination region of said examination subject that is located outside of said center of said measurement volume.

5. The method as claimed in claim 1 comprising radiating said non-selective RF excitation pulses as square-wave RF excitation pulses.

6. The method as claimed in claim 1 comprising radiating said non-selective RF excitation pulses with a duration of less than 20 microseconds.

7. The method as claimed in claim 1 comprising radiating said non-selective RF excitation pulses with a duration of less than 10 microseconds.

8. The method as claimed in claim 1 comprising radiating said non-selective RF excitation pulses with a duration of less than 5 microseconds.

9. The method as claimed in claim 1 comprising radiating said non-selective RF pulse with said adapted base frequency with a spectral curve that corresponds to a sinc function with a half-width of approximately 20% more than a reciprocal of a duration of said RF excitation pulse with said adapted base frequency.

10. The method as claimed in claim 1 wherein said examination subject comprises an examination region in which said nuclear spins are excited and from which said MR signals emanate, said examination region exhibiting a Larmor frequency that results from said combined magnetic field, and said method comprising, in said computerized control unit, automatically setting said base frequency of each non-selective RF excitation pulse to said Larmor frequency that results from said combined magnetic field.

11. A magnetic resonance (MR) apparatus comprising:
an MR data acquisition unit comprising a radio-frequency (RF) antenna, a gradient coil system, and a basic field magnet that generates a basic magnetic field in said MR data acquisition unit;
a control computer configured to control a scan of the examination subject to acquire MR data therefrom by generating and providing a pulse sequence to the MR data acquisition unit that operates the RF antenna of the MR data acquisition unit, with the examination subject therein, to radiate a plurality of non-selective radio-frequency (RF) excitation pulses into the examination subject that each has a base frequency that non-selectively excites nuclear spins in the examination subject and thereby produces MR signals resulting from the excited nuclear spins, while operating said gradient coil system to simultaneously activate a phase coding magnetic field gradient that spatially encodes the MR signals, and thereby producing a combined magnetic field in said MR data acquisition unit that is a superimposition of said basic magnetic field and said phase coding magnetic field gradient, said combined magnetic field changing during said scan due to the switching of the phase coding magnetic field gradient; and
said control computer being configured to automatically set the base frequency of each non-selective RF excitation pulse in said pulse sequence dependent on the combined magnetic field that exists at a time in said pulse sequence at which that respective non-selective RF pulse is radiated, due to the phase coding magnetic field gradient that is simultaneously switched at said time.

12. The MR apparatus of claim 11 wherein said examination subject comprises an examination region in which said nuclear spins are excited and from which said MR signals emanate, said examination region exhibiting a Larmor frequency that results from said combined magnetic field, and wherein said computerized control unit is configured to automatically set said base frequency of each non-selective RF excitation pulse to said Larmor frequency that results from said combined magnetic field.

13. A non-transitory, computer-readable data storage medium encoded with programming instructions, said data storage medium being loaded into a control computer of a magnetic resonance (MR) apparatus that comprises an MR data acquisition unit in which a basic magnetic field is generated, said programming instructions causing said control computer to:
control a scan of the examination subject to acquire MR data therefrom by generating and providing a pulse sequence to the MR data acquisition unit that operates the MR data acquisition unit, with the examination subject therein, to radiate a plurality of non-selective radio-frequency (RF) excitation pulses into the examination subject that each has a base frequency that non-selectively excites nuclear spins in the examination subject and thereby produces MR signals resulting from the excited nuclear spins, and to simultaneously activate a phase coding magnetic field gradient that spatially encodes the MR signals, and thereby producing a combined magnetic field in said MR data acquisition unit that is a superimposition of said basic magnetic field and said phase coding magnetic field gradient, said combined magnetic field changing during said scan due to the switching of the phase coding magnetic field gradient; and
automatically set the base frequency of each non-selective RF excitation pulse in said

Assignees

• Grodzki David
• Siemens Ag

Inventors

• Grodzki David

Classifications

• A61B5/055

  involving electronic [EMR] or nuclear [NMR] magnetic resonance, e.g. magnetic resonance imaging · CPC title

• G01R33/482

  using a Cartesian trajectory · CPC title

• G01R33/4824

  using a non-Cartesian trajectory · CPC title

• G01R33/5659 Primary

  caused by a distortion of the RF magnetic field, e.g. spatial inhomogeneities of the RF magnetic field (G01R33/56509, G01R33/56518, G01R33/56536 take precedence) · CPC title

• G01R33/4816

  NMR imaging of samples with ultrashort relaxation times such as solid samples, e.g. MRI using ultrashort TE [UTE], single point imaging, constant time imaging · CPC title