Fast NMR cardiac profile imaging

• US 4,995,394 A
• Filed: 08/11/1989
• Issued: 02/26/1991
• Est. Priority Date: 08/11/1989
• Status: Expired due to Term

• Current Assignee: General Electric Company
• Original Assignee: General Electric Company
• Inventors: Hardy, Christopher J., Cline, Harvey E.
• Primary Examiner(s): Jaworski, Francis
• Assistant Examiner(s): Pontius, Kevin
• Application Number:
  US07/392,315
• Time in Patent Office: 564 Days
• Field of Search: 128/653 A, 128/653 AF, 128/653, 324/309
• US Class Current: 600/410
• 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 33/4824 using a non-Cartesian trajectory
• CPC Class Codes: G01R 33/4836 using an RF pulse being spatially selective in more than one spatial dimension, e.g. a 2D pencil-beam excitation pulse
• CPC Class Codes: G01R 33/5617 using RF refocusing, e.g. RARE
• CPC Class Codes: G01R 33/56308 Characterization of motion or flow; Dynamic imaging
• CPC Class Codes: G01R 33/5676 Gating or triggering based on an MR signal, e.g. involving one or more navigator echoes for motion monitoring and correction

Abstract

A substantially continuous image, recording motion of a portion of a sample, is provided by first NMR exciting, through use of a rotating-gradient (ρ) pulse signal, a relatively narrow cylindrical region, typically with diameter less than 1 inch, of magnetization intersecting the sample to be imaged and then acquiring the NMR response signal thus excited, in the presence of a readout gradient oriented along the length of the cylindrical excitation beam and establishing position thereon. A Fourier transformation of the acquired data allows display of a real-time record of the profile of the sample along the axis of the cylindrical probe beam. The cylinder-beam axis can be oriented in an arbitrary direction by proper mixing of the excitation and readout gradient fields; use of three orthogonal gradients in a Cartesian coordinate system is presently preferred. Spatial offsetting of the cylindrical beam, from the center of the static magnetic field of the NMR imaging system, to any specific location within the system'"'"'s imaging volume, can be obtained by frequency modulation of the ρ pulse RF waveform.

Claims

1. A method for providing a nuclear-magnetic-resonance (NMR) image of movement of a selected portion of a sample, relative to a predetermined center location at the origin of a set of axes defining an imaging volume, comprising the steps of:

(a) immersing the sample in a static magnetic field formed in the imaging volume;

(b) exciting spin magnetization of nuclei in a region of the sample defined by a relatively narrow elongated probe beam;

(c) moving the probe beam to extend through the selected sample portion;

(d) acquiring a NMR response signal from the excited region, in the presence of a readout magnetic field gradient oriented along the probe beam and with a magnitude establishing the location of the selected portion therealong; and

(e) displaying said acquired NMR response signal as a profile of the sample along the beam versus time.

2. The method of claim 1, wherein steps (b)-(d) are periodically repeated, to cause the display to record the movement of the selected sample portion with respect to time.

3. The method of claim 2, wherein a heart is the sample and each repetition occurs in a repetition time interval T_R of between about 30 and about 50 millisecs.

4. The method of claim 3, wherein between about 20 and about 35 repetitions occur each second.

5. The method of claim 2, wherein between about 20 and about 50 repetitions occur each second.

6. The method of claim 2, wherein step (c) includes the steps of:

providing an excitation RF signal pulse substantially at the resonance frequency of the nuclear species to e imaged; and

simultaneously providing a gradient magnetic field undergoing reorientation in a plane selected to be perpendicular to the direction of three-dimensional orientation of the probe beam through the sample.

7. The method of claim 6, wherein the reorienting gradient magnetic field establishes a tip angle of the probe beam with respect to the imaging volume axes;

and step (c) further comprises the step of modulating the frequency of the RF excitation signal to spatially move the probe beam away from the predetermined center location.

8. The method of claim 7, further comprising the step of causing the probe beam to be of substantially cylindrical shape.

9. The method of claim 8, further comprising the step of causing the probe beam to have a substantially uniform cross-sectional profile.

10. The method of claim 8, further comprising the step of causing the probe beam to have a substantially Gaussian-cross-sectional profile.

11. The method of claim 8, wherein the probe beam has an aliasing ring at a radius R_A ;

and wherein step (d) further comprises the step of receiving the NMR response signal with a receiving antenna having an effective reception radius R less than R_A and a central axis substantially aligned with the selected sample portion.

12. The method of claim 6, further comprising the step of flow compensating the reorienting magnetic field gradients to reduce response signal contribution from fluid flowing through the probe beam.

13. The method of claim 12, further comprising the step of flow compensating the readout magnetic field gradient.

14. The method of claim 13, further comprising the step of dephasing the total magnetization in the reorienting gradient magnetic field, prior to each periodic repetition.