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US5162737A Expired / Lapsed US ⏱️ 0.0 years remaining

Multi-echo NMR imaging method

Assignee: Hitachi Healthcare Manufacturing Ltd
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Filing: 1991-12-13
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Granted: 1992-11-10
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Expires: 2011-12-13
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Abstract

Abstract A multi-echo NMR imaging method of obtaining images separated from each other with respect to two kinds of chemical shifts, typically, a fat image and a water image, includes performing the measurement of an object to be examined through a multi-echo sequence in which phase differences of θ 1 ≠nπ and θ 2 =2nπ (n=±1, ±2, ---) are respectively produced for first and second echoes between two kinds of spins to be separated from each other, deriving first and second complex images of the object from the first and second echoes, respectively, performing the measurement of a phantom exhibiting one of the chemical shifts through the multi-echo sequence and deriving third and fourth complex images of the phantom, eliminating phase errors due to a static magnetic field inhomogeneity from the first and second images using phase data of the third and fourth images respectively, and eliminating phase error due to a magnetic permeability distribution to the object.

Inventors

  • 👤 Tatsuo Nozokido
  • 👤 Etsuji Yamamoto
  • 👤 Hideki Kohno

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-11-07 20:59
CPC Classifications
G; G01; G01R; G01R33/00; G01R33/20; G01R33/44; G01R33/48; G01R33/4828; G01R33/483; G01R33/485; G01R33/54; G01R33/56; G01R33/565; G01R33/56563

Claims Analysis

Total Claims: 5
Claim 1
Independent Claim 461 words
An NMR imaging method for measuring nuclear spin information of an object using an NMR imaging system having an inspection zone to which a static magnetic field is applied, the imaging method including the steps of: i) measuring spin data of the object by disposing the object of the inspection zone and by effecting a multi-echo NMR measurement sequence to obtain first and second two-dimensional spin data sets, the multi-echo NMR measurement sequence including the steps of, a) exciting spins in the object in the inspection zone, b) applying a phase encoding gradient of a time-intensity product to the static magnetic field according to a program, c) sequentially applying first and second 180° RF pulses to the object to generate first and second Hahn echoes, d) applying a read-out gradient to the static magnetic field to generate first and second gradient echoes, respectively, corresponding to the first and the second Hahn echoes, and measuring the first and the second gradient echoes, respectively, wherein a first time difference between the first Hahn echo and the first gradient echo provide two chemical shifts of the spins in the object with a predetermined phase difference other than nπ (where n is a integer), and a second time difference between the second Hahn echo and the second gradient echo provide the two chemical shifts with a phase difference of 2nπ, and e) repeating the steps a) to d) a plurality of times while changing the time-intensity product of the phase encoding gradient to obtain the first spin data set representing the first gradient echo measured through the repetitions and the second spin data set representing the second gradient echo measured through the repetitions; ii) measuring spin data of a phantom having one of the two chemical shifts by disposing the phantom in the inspection zone and by effecting the multi-echo NMR measurement sequence to obtain third and fourth two-dimensional spin data sets; iii) obtaining first and second image data by effecting two-dimensional Fourier transformation respectively on the first and the second two-dimensional spin data sets; iv) obtaining third and fourth image data by effecting two-dimensional Fourier transformation respectively on the third and the fourth two-dimensional spin data sets; v) respectively eliminating phase error distributions due to inhomogeneity of the static magnetic field from the first and the second image data by respectively using phase distributions of the third and the fourth image data as respective compensation data and resultantly obtaining fifth and sixth image data; and vi) eliminating a phase error distribution due to a magnetic permeability distribution of the object from the fifth image data by using a phase distribution calculated from the sixth image data as compensation data and resultantly obtaining seventh image data including spin distribution information of the two chemical shifts.
Claim 2
Dependent Claim 461 words
An NMR imaging method for measuring nuclear spin information of an object using an NMR imaging system having an inspection zone to which a static magnetic field is applied, the imaging method including the steps of: i) measuring spin data of the object by disposing the object of the inspection zone and by effecting a multi-echo NMR measurement sequence to obtain first and second two-dimensional spin data sets, the multi-echo NMR measurement sequence including the steps of, a) exciting spins in the object in the inspection zone, b) applying a phase encoding gradient of a time-intensity product to the static magnetic field according to a program, c) sequentially applying first and second 180° RF pulses to the object to generate first and second Hahn echoes, d) applying a read-out gradient to the static magnetic field to generate first and second gradient echoes, respectively, corresponding to the first and the second Hahn echoes, and measuring the first and the second gradient echoes, respectively, wherein a first time difference between the first Hahn echo and the first gradient echo provide two chemical shifts of the spins in the object with a predetermined phase difference other than nπ (where n is a integer), and a second time difference between the second Hahn echo and the second gradient echo provide the two chemical shifts with a phase difference of 2nπ, and e) repeating the steps a) to d) a plurality of times while changing the time-intensity product of the phase encoding gradient to obtain the first spin data set representing the first gradient echo measured through the repetitions and the second spin data set representing the second gradient echo measured through the repetitions; ii) measuring spin data of a phantom having one of the two chemical shifts by disposing the phantom in the inspection zone and by effecting the multi-echo NMR measurement sequence to obtain third and fourth two-dimensional spin data sets; iii) obtaining first and second image data by effecting two-dimensional Fourier transformation respectively on the first and the second two-dimensional spin data sets; iv) obtaining third and fourth image data by effecting two-dimensional Fourier transformation respectively on the third and the fourth two-dimensional spin data sets; v) respectively eliminating phase error distributions due to inhomogeneity of the static magnetic field from the first and the second image data by respectively using phase distributions of the third and the fourth image data as respective compensation data and resultantly obtaining fifth and sixth image data; and vi) eliminating a phase error distribution due to a magnetic permeability distribution of the object from the fifth image data by using a phase distribution calculated from the sixth image data as compensation data and resultantly obtaining seventh image data including spin distribution information of the two chemical shifts.
Claim 3
Dependent Claim 32 words
An NMR imaging method according to claim 1, wherein the phantom has a larger section than that of the object and contains uniformly a substance exhibiting one of the two chemical shifts.
Claim 4
Dependent Claim 28 words
An NMR imaging method according to claim 1, further comprising a step of eliminating an offset phase which does not depend upon positions from the seventh image data.
Claim 5
Dependent Claim 36 words
An NMR imaging method according to claim 3, said offset phase is detected from a phase of a data of a pixel on the seventh image data at which only one of the chemical shifts exhibits.

References Cited (Backward Citations)

US4581582A Cited
US4628262A Cited
EP0226247A2 Cited
US4739266A Cited
US4760339A Cited
US4833408A Cited
EP0390175A2 Cited

USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1995-11-10 1996-05-11 1996-11-10 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 1999-11-10 2000-05-11 2000-11-10 $3760.00 Window Closed / Lapsed
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