IP Library Granted Patent US 9,662,037
Granted Patent B2
US 9,662,037 · App. 13/354,775 · Granted May 30, 2017

Magnetic resonance imaging apparatus and magnetic resonance imaging method

Inventors: Naho Takahashi (Otawara, JP); Masao Yui (Otawara, JP)
Assignee: TOSHIBA MEDICAL SYSTEMS CORPORATION
A61B5/055A61B5/0037G01R33/48
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Quick Facts
Patent No.
US 9,662,037
App. No.
13/354,775
Granted
May 30, 2017
Kind
B2
Abstract

According to one embodiment, a magnetic resonance imaging apparatus includes a spectrum acquisition unit, a resonance frequency acquisition unit and an imaging unit. The spectrum acquisition unit is configured to acquire frequency spectra of magnetic resonance signals from an object while changing a suppression effect or an enhancing effect of signals from a specific material. The resonance frequency acquisition unit is configured to obtain a resonance frequency of the specific material or another material based on an index representing a difference in intensities of signals from the specific material or the another material between the frequency spectra. The imaging unit is configured to perform imaging using a radio frequency pulse having a center frequency set to the resonance frequency of the specific material or the another material.

Claims (28)

1. A magnetic resonance (MR) imaging apparatus comprising:

MRI system components including static and gradient magnetic field generators, at least one radio frequency (RF) coil, an RF transmitter, an RF receiver and at least one computer configured to control said components to

acquire frequency spectra including a first frequency spectrum of first MR signals and a second frequency spectrum of second MR signals from an object, said spectra exhibiting a changing suppression effect or a changing enhancing effect of signals from a specific material;

obtain a resonance frequency of the specific material or another material using a frequency spectrum, for obtaining the resonance frequency of the specific material or the another material, selected from the first frequency spectrum and the second frequency spectrum based on an index representing a difference in intensities of signals from the specific material or the another material between the first frequency spectrum and the second frequency spectrum; and

perform MR imaging using a radio frequency pulse having a center frequency set to the resonance frequency of the specific material or the another material.

2. The magnetic resonance imaging apparatus of claim 1 , wherein

the first and second frequency spectrums having fat suppression effects that are mutually different are acquired by (a) changing a flip angle of a fat saturation pulse or (b) applying or not applying a fat saturation pulse, and

a resonance frequency of water is obtained using a frequency spectrum showing a larger fat suppression effect in a case where an index representing a difference in intensity of signals from fat is determined to be small by threshold processing and a resonance frequency of the fat is obtained using a frequency spectrum showing a smaller fat suppression effect in a case where the index is determined to be large by the threshold processing to obtain the resonance frequency of the water based on the obtained resonance frequency of the fat.

3. The magnetic resonance imaging apparatus of claim 2 , wherein

a difference or a rate between integral values of curves representing intensities of signals from the fat is used as the index.

4. The magnetic resonance imaging apparatus of claim 2 , wherein

a difference or a rate between peaks of intensities of signals from the fat is used as the index.

5. The magnetic resonance imaging apparatus of claim 2 , wherein said at least one computer is further configured

to determine whether the resonance frequency of the water was obtained with a predetermined accuracy using the frequency spectrum showing the larger fat suppression effect so as not to acquire the frequency spectrum showing the smaller fat suppression effect in a case where it was determined that the resonance frequency of the water had been obtained with the predetermined accuracy.

6. The magnetic resonance imaging apparatus of claim 1 , wherein

the first and second frequency spectrums showing mutually different degrees in suppression or enhancing effect of signals from the specific material are acquired based on a difference in longitudinal relaxation time between the specific material and the another material.

7. The magnetic resonance imaging apparatus of claim 1 , wherein,

a resonance frequency of water is obtained based on signal rates in first frequency bands between frequency spectra showing mutually different fat suppression effects and a ratio of the signal rates between the first frequency bands and second frequency bands respectively distant from the first frequency bands by a predetermined frequency, the frequency bands corresponding to respective maximum values of the frequency spectra.

8. A magnetic resonance (MR) imaging apparatus comprising:

MRI system components including static and gradient magnetic field generators, at least one radio frequency (RF) coil, an RF transmitter, an RF receiver and at least one computer configured to control said components to

acquire a frequency spectrum of magnetic resonance signals from an object with suppressing or enhancing signals from a specific material;

obtain a resonance frequency of the specific material or another material by shifting the acquired frequency spectrum in a frequency direction based on an index representing an equality degree or an inequality degree between the frequency spectrum and a reference frequency spectrum; and

perform MR imaging using a radio frequency pulse having a center frequency set to the resonance frequency of the specific material or the another material.

9. A magnetic resonance (MR) imaging method comprising:

using MRI system components including static and gradient magnetic field generators, at least one radio frequency (RF) coil, an RF transmitter, an RF receiver and at least one computer configured to control said components to effect

acquiring a first frequency spectrum of first MR signals and a second frequency spectrum of MR signals from an object, said spectra exhibiting a changing suppression effect or a changing enhancing effect of signals from a specific material;

obtaining a resonance frequency of the specific material or another material using a frequency spectrum, for obtaining the resonance frequency of the specific material or the another material, selected from the first frequency spectrum and the second frequency spectrum based on an index representing a difference in intensities of signals from the specific material or the another material between the first and second frequency spectrums; and

performing MR imaging using a radio frequency pulse having a center frequency set to the resonance frequency of the specific material or the another material.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 27, 2016
From: KABUSHIKI KAISHA TOSHIBA
To: TOSHIBA MEDICAL SYSTEMS CORPORATION
Reel/Frame 038735/0277 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 20, 2012
From: TAKAHASHI, NAHO; YUI, MASAO
To: KABUSHIKI KAISHA TOSHIBA; TOSHIBA MEDICAL SYSTEMS CORPORATION
Reel/Frame 027568/0838 →
Priority Claims (1)
JP 2010-235010 · Oct 19, 2010 · national
Continuity (2)
Continuation PCTJP2011073018 · Oct 5, 2011
Related Publication 20120119740A1 · May 17, 2012