U.S. patents available from 1976 to present.
U.S. patent applications available from 2005 to present.

Rapid magnetic resonance imaging using multiple phase encoded spin echoes in each of plural measurement cycles

Patent 4684891 Issued on August 4, 1987. Estimated Expiration Date: Icon_subject July 31, 2005. Estimated Expiration Date is calculated based on simple USPTO term provisions. It does not account for terminal disclaimers, term adjustments, failure to pay maintenance fees, or other factors which might affect the term of a patent.

Patent References

Gyromagnetic resonance fourier transform zeugmatography
Patent #: 4070611
Issued on: 01/24/1978
Inventor: Ernst

Method and apparatus for mapping lines of nuclear density within an object using nuclear magnetic resonance
Patent #: 4297637
Issued on: 10/27/1981
Inventor: Crooks ,   et al.

Method and apparatus for rapid NMR imaging of nuclear densities within an object
Patent #: 4318043
Issued on: 03/02/1982
Inventor: Crooks ,   et al.

Nuclear magnetic resonance systems
Patent #: 4355282
Issued on: 10/19/1982
Inventor: Young ,   et al.

Method and apparatus for rapid NMR imaging of nuclear parameters with an object
Patent #: 4471305
Issued on: 09/11/1984
Inventor: Crooks ,   et al.

Vivo P-31 NMR imaging of phosphorus metabolites
Patent #: 4567440
Issued on: 01/28/1986
Inventor: Haselgrove

Method for visualization of in-plane fluid flow by proton NMR imaging
Patent #: 4570119
Issued on: 02/11/1986
Inventor: Wehrli ,   et al.

Method for rapid acquisition of NMR data Patent #: 4587489
Issued on: 05/06/1986
Inventor: Wehrli

Inventor

Assignee

Application

No. 06/760832 filed on 07/31/1985

US Classes:

324/309, To obtain localized resonance within a sample324/307Using a nuclear resonance spectrometer system

Examiners

Primary: Tokar, Michael

Attorney, Agent or Firm

International Classes

G01R 33/54 (20060101)
G01R 33/561 (20060101)

Abstract

Slice selective 90° and plural subsequent 180° NMR RF pulses are utilized to elicit a train of NMR spin echoes from a given slice or "planar volume" of the object under test in each of plural measurement cycles. Spatial information is encoded within the spin echo by imposing a Gx gradient during each spin echo readout. Phase encoding in a second Gy dimension is achieved by using (1) a cycle-dependent ଲGy gradient at least once during each NMR measurement cycle and (2) further δGy magnetic gradient pulses in association with some or all of the individual spin echo responses within each measurement cycle. The two different types of Gy gradient pulses are dimensioned and timed so as to result in the desired number of phase encoded spin echo signals which subsequently can be arranged in a linearly increasing progression of phase encoding so as to be usable in a two-dimensional Fourier transformation process to produce an NMR image. Because the spin echo data are taken at different times of echo occurrences within a given measurement cycle, T2 artifact may be present in such an image. However T2 correction may be provided by calculating T2 and scaling all of the time domain spin echo data to a single common equivalent time of echo occurrence before performing the final two-dimensional Fourier transformation process which results in a final T2-corrected NMR image.

Other References

  • Kumar et al, J. Mag., Res. 18, 69-83 (1975)
  • Mansfield et al, J. Mag., Res. 29. 335-373 (1978)
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