Moving gradient zeugmatography

• US 4,307,343 A
• Filed: 08/20/1979
• Issued: 12/22/1981
• Est. Priority Date: 08/20/1979
• Status: Expired

• Current Assignee: General Electric Company
• Original Assignee: General Electric Company
• Inventors: Likes, Richard S.
• Primary Examiner(s): Tokar, Michael J.
• Application Number:
  US06/067,697
• Time in Patent Office: 855 Days
• Field of Search: 324/309
• US Class Current: 324/307
• CPC Class Codes: G01R 33/446 Multifrequency selective RF pulses, e.g. multinuclear acquisition mode spatially selective RF pulses G01R33/4833
• CPC Class Codes: G01R 33/5615 Echo train techniques involving acquiring plural, differently encoded, echo signals after one RF excitation, e.g. using gradient refocusing in echo planar imaging [EPI], RF refocusing in rapid acquisition with relaxation enhancement [RARE] or using both RF and gradient refocusing in gradient and spin echo imaging [GRASE]

Abstract

Nuclear magnetic resonance phenomena are employed to generate a two dimensional image of a thin planar slice through a body under investigation. The apparatus herein operates to determine the spin density distribution in a planar slab within the body which typically comprises a biological organism. Each pixel in the resulting image is distinguished by applying time-varying magnetic field gradients so that the frequency history of the spins in each pixel is uniquely distinguishable. Additionally, novel radio frequency excitation means assure selective excitation within the planar slab.

Claims

1. A nuclear magnetic resonance apparatus for determining spin density distribution in a thin planar slab of an object under examination containing nuclear spins, said body being oriented with respect to orthogonal x and y coordinate directions defined therein and also to a z coordinate direction orthogonal to said slab and to said x and y coordinates within said slab, said apparatus comprising:

excitation means for selectively exciting said nuclear spins in said slab, said excitation means including means for applying to said object for a predetermined time period an excitation magnetic field having a gradient in the z-axis direction, said gradient being defined by a function G(t) not having a DC component, said excitation means also including means for applying a pulse of RF energy to said object during the time that said excitation magnetic field is applied, said pulse having an envelope defined by a function h₁ (t)=h₁ γ

G(t)f(K/K₀)(T₀ /K₀) wherein h₁ is a constant, T₀ is a point in time when G(t) is approximately zero, and f is a window function, so that said excited nuclear spins undergo a radiative free induction decay following termination of said excitation and so that nuclear spins in other regions of said object are substantially unexcited;

means for applying to said object a spatial differentiation magnetic field H(x,y,t), during at least a portion of the free induction decay of said excited nuclear spins, said magnetic field having the form H₀ +G₁ (t)x+G₂ (t)y;

means for receiving radiated electromagnetic energy produced by said free induction decay and converting said energy to a time-varying electric signal representative of the magnitude of said energy; and

means for operating on said electrical signal to generate therefrom signals representative of the spin density distribution in said slab.

2. The nuclear magnetic resonance apparatus of claim 1 in which G(t)=G₀ ((T₀² -t²)/T₀²)exp[-(t/T₀)² /2].

3. The nuclear magnetic resonance apparatus of claim 1 in which said receiving means comprises a coil disposed about said object.

4. The nuclear magnetic resonance apparatus of claim 1 in which said radio frequency pulse means includes a transmission coil disposed about the object.

5. The nuclear magnetic resonance apparatus of claim 4 in which said radio frequency pulse transmission coil is the same as the means for receiving radiated electromagnetic energy.

6. The nuclear magnetic resonance apparatus of claim 4 in which said radio frequency pulse transmission coil is disposed within and axially perpendicular to a coil operating as the means for receiving the radiated electromagnetic energy.

7. The nuclear magnetic resonance apparatus of claim 1 in which said functions G₁ (t) and G₂ (t) are selected to produce K-space trajectories which are Lissajous figures.

8. The nuclear magnetic resonance apparatus of claim 1 in which said functions G₁ (t) and G₂ (t) are selected to produce K-space trajectories which are rosettes.

9. The nuclear magnetic resonance apparatus of claim 1 in which said functions G₁ (t) and G₂ (t) are selected to produce K-space trajectories which are Archimedian spirals.

10. The nuclear magnetic resonance apparatus of claim 1 in which said functions G₁ (t) and G₂ (t) are selected to produce K-space trajectories which are concentric circles.

11. The nuclear magnetic resonance apparatus of claim 1 in which said spatial differentiation magnetic field H(x,y,t) defines a plurality of K-space trajectories, wherein said trajectories provide a complete and uniform coverage of K-space and wherein the dwell time in each region of K-space is approximately equal so that a detailed image of the entire portion of said object lying in the K-space plane is produced.

12. The nuclear magnetic resonance apparatus of claim 1 in which said spatial differentiation magnetic field H(x,y,t) defines a plurality of K-space trajectories, wherein said K-space trajectories concentrate on and have greater dwell time in selected region of K-space, thus enhancing the image contrast in said selected regions.

13. The nuclear magnetic resonance apparatus of claim 1 wherein the relation of the maximum absolute value G of said function G(t) to the peak amplitude H₁ of said function h₁ (t) is given by the expression (G)(Δ

Z)≈

H₁.