IP Library Granted Patent US 10,638,950
Granted Patent B2
US 10,638,950 · App. 15/543,381 · Granted May 5, 2020

Magnetic resonance imaging apparatus, static magnetic field homogeneity adjustment method, program, and computer

Inventors: Takuya Fujikawa (Tokyo, JP); Mitsushi Abe (Tokyo, JP); Kenji Sakakibara (Tokyo, JP); Hikaru Hanada (Tokyo, JP)
Assignee: HITACHI, LTD.
A61B5/055G01R33/3873G01R33/385G01R33/3815
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Quick Facts
Patent No.
US 10,638,950
App. No.
15/543,381
Granted
May 5, 2020
Kind
B2
Abstract

In order to provide a static magnetic field homogeneity adjustment method capable of reducing an arrangement amount of magnetic pieces and achieving desired magnetic field homogeneity with high accuracy in magnetic field homogeneity adjustment, there is provided a static magnetic field homogeneity adjustment method in an imaging space of computing positions of a plurality of magnetic pieces separated from the imaging space through shimming computation with respect to a static magnetic field in the imaging space generated by a magnetic field generation device, and disposing the plurality of magnetic pieces at the positions obtained through the shimming computation, the method including an adjustment step of imposing restriction that a polarity of a magnetic field distribution generated in the imaging space by the magnetic pieces disposed at the positions is either positive or negative during the shimming computation, and adjusting the static magnetic field homogeneity.

Claims (37)

1. A static magnetic field homogeneity adjustment method for a magnetic resonance imaging apparatus in an imaging space of computing positions of a plurality of magnetic pieces separated from the imaging space through shimming computation with respect to a static magnetic field in the imaging space generated by a magnetic field generation device, and disposing the plurality of magnetic pieces at the positions obtained through the shimming computation, the method comprising:

an adjustment step of imposing restriction that a polarity of a magnetic field distribution generated in the imaging space by the magnetic pieces disposed at the positions is either positive or negative during the shimming computation, and adjusting the static magnetic field homogeneity,

wherein, in a case where a direction of magnetic moment of the magnetic pieces is parallel to a direction of the static magnetic field, positions of the magnetic pieces where the magnetic pieces generate a negative magnetic field distribution in the imaging space are selected.

2. A static magnetic field homogeneity adjustment method for a magnetic resonance imaging apparatus in an imaging space of computing positions of a plurality of magnetic pieces separated from the imaging space through shimming computation with respect to a static magnetic field in the imaging space generated by a magnetic field generation device, and disposing the plurality of magnetic pieces at the positions obtained through the shimming computation, the method comprising:

an adjustment step of imposing restriction that a polarity of a magnetic field distribution generated in the imaging space by the magnetic pieces disposed at the positions is either positive or negative during the shimming computation, and adjusting the static magnetic field homogeneity,

wherein, in a case where a direction of magnetic moment of the magnetic pieces is orthogonal to a direction of the static magnetic field, positions of the magnetic pieces where the magnetic pieces generate a positive magnetic field distribution in the imaging space are selected.

3. The static magnetic field homogeneity adjustment method for a magnetic resonance imaging apparatus according to claim 1 ,

wherein a boundary of selected positions of the magnetic pieces is a boundary at which positive and negative magnetic field distributions generated in the imaging space by the magnetic pieces satisfy the following equation:

3

M

z

·

Z

2

r

5

-

Mz

r

3

=.

where Z is a position in a static magnetic field direction (Z axis direction), r is a distance from magnetic moment, and Mz is magnetic moment [Am 2 ] in the static magnetic field direction (Z axis direction).

4. A static magnetic field homogeneity adjustment method for a magnetic resonance imaging apparatus in an imaging space of computing positions of a plurality of magnetic pieces separated from the imaging space through shimming computation with respect to a static magnetic field in the imaging space generated by a magnetic field generation device, and disposing the plurality of magnetic pieces at the positions obtained through the shimming computation, the method comprising:

an adjustment step of imposing restriction that a polarity of a magnetic field distribution generated in the imaging space by the magnetic pieces disposed at the positions is either positive or negative during the shimming computation, and adjusting the static magnetic field homogeneity,

wherein, in the adjustment step of disposing the magnetic pieces, each location from a bore opening of the magnetic field generation device is selected so that a magnetic piece is not disposed therein, and a negative region is estimated by evaluating magnetic field homogeneity predicted after the adjustment step is completed, and a magnetic piece amount used for the adjustment step is changed.

5. A magnetic resonance imaging apparatus comprising:

a magnetic field generation device that is provided with an electromagnet forming a static magnetic field in an imaging space; and

magnetic body holding members in which a plurality of depressions for accommodation of magnetic pieces for magnetic field adjustment are arranged on a surface portion of the electromagnet on the imaging space side,

wherein the density of an amount of magnetic pieces accommodated in a portion of each of the magnetic body holding members close to the imaging space is higher than the density of an amount of magnetic pieces in a portion thereof distant from the imaging space,

wherein the magnetic field generation device includes a cylindrical electromagnet forming the imaging space in a cylindrical inner space,

wherein the magnetic body holding members are distributed on an inner circumferential surface of the electromagnet, and each of the magnetic body holding members is provided with a plurality of depressions which are disposed in an axial direction and accommodate the magnetic pieces in a longitudinal direction, and

wherein the depressions are not formed over a set length from both ends in some of the magnetic body holding members.

6. The magnetic resonance imaging apparatus according to claim 5 ,

wherein, in some of the magnetic body holding members, at least a length of one end side where the depressions are not formed is shorter than a length of the other side.

Assignments (5)
MERGER Recorded Jan 10, 2025
From: FUJIFILM HEALTHCARE CORPORATION
To: FUJIFILM CORPORATION
Reel/Frame 069869/0940 →
MERGER Recorded Oct 11, 2024
From: FUJIFILM HEALTHCARE CORPORATION
To: FUJIFILM CORPORATION
Reel/Frame 070607/0950 →
CORRECTIVE ASSIGNMENT TO CORRECT THE THE PROPERTY AND APPLICATION NUMBERS PREVIOUSLY RECORDED AT REEL: 058026 FRAME: 0559. ASSIGNOR(S) HEREBY CONFIRMS THE ASSIGNMENT. Recorded Jan 31, 2022
From: HITACHI LTD.
To: FUJIFILM HEALTHCARE CORPORATION
Reel/Frame 058917/0853 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Nov 4, 2021
From: HITACHI, LTD.
To: FUJIFILM HEALTHCARE CORPORATION
Reel/Frame 058026/0559 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jul 13, 2017
From: FUJIKAWA, TAKUYA; ABE, MITSUSHI; SAKAKIBARA, KENJI; HANADA, HIKARU
To: HITACHI, LTD.
Reel/Frame 043000/0142 →
Priority Claims (1)
JP 2015-034786 · Feb 25, 2015 · national
Continuity (1)
Related Publication 20170354343A1 · Dec 14, 2017