Magnetic resonance apparatus and operating method with adjustment of the excitation angle dependent on data acquisition field of view

Patent metadata

Field	Value
Publication number	US-10996307-B2
Application number	US-201916438967-A
Country	US
Kind code	B2
Filing date	Jun 12, 2019
Priority date	Jun 12, 2018
Publication date	May 4, 2021
Grant date	May 4, 2021

Abstract

In a magnetic resonance tomography (MRT) apparatus and operating method, a field of view for imaging a target object is acquired. A relative position of this field of view in relation to a receiving space of the MRT scanner, in which the target object is received, is then automatically determined. A radio-frequency (RF) pulse to be used by the MRT scanner for imaging the target object is then automatically adjusted depending on this relative position. An excitation angle produced in the field of view by the RF pulse is changed compared to the use of the corresponding unadjusted RF pulse.

First claim

The invention claimed is:

1. A method for operating a magnetic resonance tomography (MRT) apparatus comprising an MRT data acquisition scanner having a receiving space for receiving a target object from which MRT data are to be acquired by executing an MRT data acquisition protocol, provided to a control computer of said MRT apparatus, said MRT data acquisition protocol comprising at least one radio-frequency (RF) pulse, said method comprising:
providing said computer with a specification of a field of view that encompasses a portion of said receiving space from which said MRT data are to be acquired from said target object;
in said computer, automatically determining a relative position of the field of view in relation to said receiving space of the MRT scanner; and
in said computer, automatically adjusting said at least one RF pulse dependent on the determined relative position of the field of view, so as to change an excitation angle produced by said at least one RF pulse in said field of view, compared to an excitation angle produced by the original RF pulse in said MRT data acquisition protocol.

2. A method as claimed in claim 1 comprising changing an amplitude of said RF pulse while maintaining a duration of said RF pulse unchanged.

3. A method as claimed in claim 1 comprising making a larger change to said RF pulse as said specification of said field of view shows that said field of view is closer to an edge of said receiving space.

4. A method as claimed in claim 1 comprising:
from said specification of said field of view, automatically determining a loading that exists in said receiving space;
automatically determining an expected field strength of B 1 field produced by said RF pulse in said field of view, dependent on said loading; and
changing said RF pulse dependent on a difference between the expected B 1 field strength and a specified target field strength in said MRT data acquisition protocol, so as to align said excitation angle resulting with the expected B 1 field strength with a specified target excitation angle produced by said target field strength.

5. A method as claimed in claim 1 wherein said MRT data acquisition protocol comprises a plurality of pulses, and changing all of said plurality of pulses in a same way as said at least one RF pulse.

6. A method as claimed in claim 1 wherein said MRT data acquisition protocol comprises a plurality of pulses, with only a subset of said plurality pulses being excitation pulses, and changing all excitation pulses in said subset in a same way as said at least one RF pulse.

7. A method as claimed in claim 1 wherein said MRT data acquisition protocol comprises a plurality of pulses, with only a subset of said plurality pulses being refocusing pulses, and changing all refocusing pulses in said subset in a same way as said at least one RF pulse.

8. A method as claimed in claim 1 wherein said MRT data acquisition protocol comprises a plurality of RF pulses, including fat saturation pulses, and changing all of said RF pulses, except said fat saturation pulses, in a same way as said at least one RF pulse is changed.

9. A method as claimed in claim 1 comprising changing said RF pulse according to a specified function selected from the group consisting of a quadratic function that is dependent on a spatial variable in said field of view, a polynomial function that is higher than a second degree, a step function, and an exponential function.

10. A magnetic resonance tomography (MRT) apparatus comprising:
an MRT data acquisition scanner comprising a receiving space in which a target object is received;
a control computer configured to operate the MRT data acquisition scanner in order to execute an MRT data acquisition protocol so as to acquire MRT data from the target object, said MRT data acquisition protocol comprising at least one RF pulse;
a detector that detects and provides said computer with a specification of a field of view that encompasses a portion of said receiving space from which said MRT data are to be acquired from said target object;
said computer being configured to automatically determine a relative position of the field of view in relation to said receiving space of the MRT scanner; and
said computer being configured to automatically adjust said at least one RF pulse dependent on the determined relative position of the field of view, so as to change an excitation angle produced by said at least one RF pulse in said field of view, compared to an excitation angle produced by the original RF pulse in said MRT data acquisition protocol.

11. A non-transitory, computer-readable data storage medium encoded with programming instructions, said storage medium being loaded into a control computer of a magnetic resonance tomography (MRT) apparatus that comprises an MRT data acquisition scanner having a receiving space in which a target object is received in order to acquire MRT data from the target object according to an MRT data acquisition protocol that comprises at least one RF pulse, said programming instructions causing said control computer to:
receive a specification of a field of view that encompasses a portion of said receiving space from which said MRT data are to be acquired from said target object;
determine a relative position of the field of view in relation to said receiving space of the MRT scanner; and
adjust said at least one RF pulse dependent on the determined relative position of the field of view, so as to change an excitation angle produced by said at least one RF pulse in said field of view, compared to an excitation angle produced by the original RF pulse in said MRT data acquisition protocol.

Assignees

• Siemens Healthcare Gmbh

Inventors

• Carinci Flavio
• Ferguson George William
• Koehler Michael
• Ritter Dieter
• Paul Dominik

Classifications

• A61B5/055

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

• G01R33/32

  Excitation or detection systems, e.g. using radio frequency signals · CPC title

• G01R33/5617

  using RF refocusing, e.g. RARE · CPC title

• G01R33/5659

  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

• G01R33/4831

  using B1 gradients, e.g. rotating frame techniques, use of surface coils · CPC title