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

Magnetic resonance imaging apparatus

Patent 5341099 Issued on August 23, 1994. Estimated Expiration Date: Icon_subject March 31, 2013. 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

Conjugate symmetry magnetic resonance imaging
Patent #: 4780675
Issued on: 10/25/1988
Inventor: DeMeester ,   et al.

Scan time reduction using conjugate symmetry and recalled echo
Patent #: 4833407
Issued on: 05/23/1989
Inventor: Holland ,   et al.

Three dimensional volume imaging with conjugate symmetrization
Patent #: 4851779
Issued on: 07/25/1989
Inventor: DeMeester ,   et al.

MR imaging method and apparatus
Patent #: 4912412
Issued on: 03/27/1990
Inventor: Suzuki, et al.

Conjugate symmetry magnetic resonance imaging
Patent #: 4912413
Issued on: 03/27/1990
Inventor: DeMeester, et al.

Image reconstruction method in NMR imaging
Patent #: 4993075
Issued on: 02/12/1991
Inventor: Sekihara, et al.

Correction of NMR data acquired by an echo-planar technique Patent #: 5151656
Issued on: 09/29/1992
Inventor: Maier, et al.

Inventor

Application

No. 040854 filed on 03/31/1993

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

Foreign Patent References

  • 0280310 EP. 08/13/1988
  • 0306135 EP. 03/13/1989
  • 0329299 EP. 08/13/1989
  • 1131649 JP. 05/13/1989
  • 241138 JP. 02/13/1990

International Class

G01R 033/20

Foreign Application Priority Data

1992-03-31 JP

Abstract

Data is produced from asymmetrical echo data, and an MR image is reconstructed from the data thus produced. Namely, inverse Fourier transformation is performed on center echo data, thereby producing phase data. The phase data is inverted in polarity, thereby producing polarity-inverted phase data. Fourier transformation is performed on the polarity-inverted phase data in a readout direction, producing phase-correction data. Inverse Fourier transformation is performed on the asymmetrical echo data in an encode direction. The phase-correction data and the echo data are convoluted in the readout direction, thereby producing echo-data free of phase distortion. Unmeasured echo data is inferred from the convoluted data by utilizing complex conjugate property of the echo data. Inverse Fourier transformation is performed on the convoluted data and the inferred data in the readout direction, thereby producing an image free of phase distortion.

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