Imaging apparatus using nuclear magnetic resonance

• US 4,625,171 A
• Filed: 02/14/1984
• Issued: 11/25/1986
• Est. Priority Date: 02/14/1983
• Status: Expired due to Fees

• Current Assignee: Hitachi Medical Corporation (Hitachi, Ltd.)
• Original Assignee: Hitachi, Ltd.
• Inventors: Kohno, Hideki, Kuroda, Masao, Sekihara, Kensuke
• Primary Examiner(s): Levy, Stewart J.
• Assistant Examiner(s): O'Shea, Kevin D.
• Application Number:
  US06/579,967
• Time in Patent Office: 1,015 Days
• Field of Search: 324/300, 324/307, 324/309, 324/310, 324/312, 324/320, 324/313, 364/413, 364/414, 364/415, 358/166, 378/19, 378/901
• US Class Current: 324/312
• CPC Class Codes: G01R 33/56518 due to eddy currents, e.g. caused by switching of the gradient magnetic field
• 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

Abstract

An NMR imaging apparatus for reconstructing a cross section of a body to be inspected, by the projection-reconstruction method. That is, an apparatus for forming the above cross section in such a manner that the nuclear magnetic resonance is caused by the to-be-inspected body in the resulting magnetic field of a static magnetic field and a rotatable gradient field, a projection of the to-be-inspected body is detected at each rotational positions of the gradient field, and the cross section is reconstructed using the above projection. The apparatus comprises memories for previously storing therein data indicating the distorsion of magnetic field such as the non-uniformity of the static magnetic field and the non-linearity of the gradient field, in order to perform the coordinate calculation in the back projection, using the data stored in the memories.

Claims

1. An imaging apparatus for obtaining a nuclear spin distribution image of an object along a two-dimensional section, comprising:

means for generating a static magnetic field which has an intensity error distribution along said two-dimensional section;

exciting means for repeatedly exciting nuclear spins in said object by repeatedly applying a pulsive high frequency magnetic field;

means for generating a gradient magnetic field successively along each of a plurality of different directions across said two-dimensional section to produce frequency dispersion of nuclear spins along each of the directions;

signal detecting means for detecting nuclear magnetic resonance signals induced during generation of said gradient magnetic field for a plurality of different directions thereof;

memory means for storing data of said intensity error distribution of said static magnetic field;

computer means for performing operations for each of said nuclear magnetic resonance signals detected by said signal detecting means to reconstruct an image in accordance with at least data read out from said memory means, said computer means performing the operations of analyzing a frequency spectrum of each of said nuclear magnetic resonance signals to obtain a projection along a frequency axis, and projecting back a value of said projection at each frequency to each picture point of said image to be reconstructed, said frequency being a resonance signal at said image point, said computer means correcting a frequency error of said frequency caused by said intensity error distribution of said static magnetic field in accordance with data read out from said memory means; and

display means responsive to said computer means for displaying the reconstructed image.

2. An imaging apparatus using the nuclear magnetic resonance according to claim 1, wherein said memory means includes a first memory for storing data of said intensity error distribution of said static magnetic field and a second memory for storing data with respect to the non-linearity of said gradient field, said computer means correcting said nuclear magnetic resonance signal by both said data read out from said first memory and said second memory.

3. An imaging apparatus using the nuclear magnetic resonance according to claim 1, wherein said memory means stores therein as the data of the intensity error distribution of said static magnetic field data of the derivative Δ

H (x, z) of the intensity of said static magnetic field from a predetermined value H_o at each (x, z) of picture points on an image, on which said nuclear magnetic resonance signal is back-projected.

4. An imaging apparatus using the nuclear magnetic resonance according to claim 3, wherein said computer means projects back the value I.sub.θ

(f_B '"'"') of said nuclear magnetic resonance signal at a corrected frequency f_B '"'"' which is given by the following equation on a corresponding one (x, z) of said picture points ##EQU22## where f_c =Δ

H_o /2π

, f.sub.ε

=γ

Δ

H (x, z)/2π

, γ

is a gyromagnetic ratio, G is an increment of the intensity of said gradient field per unit length, and θ

is an angle between a z-axis and the direction of the intensity gradient of said gradient field.

5. An imaging apparatus using the nuclear magnetic resonance according to claim 4, wherein said computer means calculate a value I.sub.θ

(f_m '"'"') of said nuclear magnetic resonance signal from discrete detection signals by the linear interpolation method.

6. An imaging apparatus using the nuclear magnetic resonance according to claim 2, wherein said second memory stores said data with respect to the non-linearity of said gradient field as coefficients of a polynominal, with which the intensity distrubution of said gradient field is approximated.

7. A method for obtaining a nuclear spin distribution image of an object along a two-dimensional section, comprising the steps of:

generating a static magnetic field;

detecting an intensity error distribution of said static magnetic field along said two-dimensional section and storing data of said intensity error distribution in a memory means;

repeatedly exciting nuclear spins in said object within said static magnetic field;

generating a gradient magnetic field successively along each of a plurality of different directions across said two-dimensional section to produce frequency dispersion of nuclear spins along each direction;

detecting nuclear magnetic signals induced during said gradient magnetic field for a plurality of different directions thereof;

analyzing frequency spectrums of respective nuclear magnetic resonance signals to obtain respective projections along a frequency axis;

projecting back respective values of said respective projections at respective frequencies to respective picture points of an image to be reconstructed, said respective frequencies being respective resonance signals at said respective image points, and correcting frequency errors of said frequencies caused by said intensity error distribution of said static magnetic field in accordance with date read out from said means; and

displaying back-projected values at respective image points.