← Back to Patent Explorer
US4682108A Expired / Lapsed US ⏱️ 0.0 years remaining

Magnetic resonance equipment for the production of images of a test object

Assignee: Siemens AG
•
Filing: 1985-07-26
•
Granted: 1987-07-21
•
Expires: 2005-07-26
📄 Original PDF 🌐 Google Patents 🔄 Sync Now

Abstract

Abstract The disclosure relates to nuclear spin tomography equipment in which means (22, 24) are provided for the control of the acquisition of the Fourier rows of the measurement matrix as a function of a respiration signal. The equipment includes a Fourier row counter (25) which influences a circuit (26) that controls the measurement signal acquisition. In a first embodiment of the invention the measurement signal acquisition is always released for all rows outside a predetermined region, but is a function of the respiration phase signal inside this region. The predetermined row region may comprise approximately 10% of all rows to be measured and should lie symmetrically about the center of the matrix. A further reduction of the measuring time is realized, according to another embodiment of the invention, by dispensing altogether with measurement in the row edge region of the matrix.

Inventors

  • 👤 Eckart Stetter
  • 👤 Helmut Reichenberger
  • 👤 Siegfried Schneider
  • 👤 Axel Wirth

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-10-27 23:28
CPC Classifications
G; G01; G01R; G01R33/00; G01R33/20; G01R33/44; G01R33/48; G01R33/54; G01R33/56; G01R33/567; G01R33/5673

Claims Analysis

Total Claims: 12
Claim 1
Independent Claim 267 words
Apparatus for producing images of a test object using nuclear magnetic resonance, at least a portion said test object being subject to physical motion, said apparatus comprising: (a) first means for applying magnetic primary and gradient fields to the test object and for detecting deflection of nuclear spins of the test object from their equilibrium position by a radio-frequency magnetic excitation pulse, said first means producing a plurality of time-sequential measurement signals representative of said nuclear spin deflection in response to a respective plurality of excitation pulses time-sequentially applied with corresponding gradient fields; (b) second means, responsive to said produced measurement signals, for calculating an image of a cross-sectional slice of the test object by Fourier transformation from a matrix of Fourier rows, each Fourier row being calculated from at least one of said time-sequential measurement signals as a projection of the nuclear spins on a frequency axis caused by the plurality of magnetic field gradients in said slice; (c) third means for generating a motion signal representative of said physical motion of said portion of the test object; (d) fourth means, coupled to said second means, for counting Fourier rows; and (e) fifth means, responsive to said fourth means and coupled to said second and third means, for controlling the calculation of said image such that said time-sequential measurement signals are continuously produced for use by said second means for the calculation of Fourier rows outside a predetermined region of the rows in said matrix, but are intermittently produced for use by said second means as a function of said motion signal when within said region.
Claim 2
Dependent Claim 267 words
Apparatus for producing images of a test object using nuclear magnetic resonance, at least a portion said test object being subject to physical motion, said apparatus comprising: (a) first means for applying magnetic primary and gradient fields to the test object and for detecting deflection of nuclear spins of the test object from their equilibrium position by a radio-frequency magnetic excitation pulse, said first means producing a plurality of time-sequential measurement signals representative of said nuclear spin deflection in response to a respective plurality of excitation pulses time-sequentially applied with corresponding gradient fields; (b) second means, responsive to said produced measurement signals, for calculating an image of a cross-sectional slice of the test object by Fourier transformation from a matrix of Fourier rows, each Fourier row being calculated from at least one of said time-sequential measurement signals as a projection of the nuclear spins on a frequency axis caused by the plurality of magnetic field gradients in said slice; (c) third means for generating a motion signal representative of said physical motion of said portion of the test object; (d) fourth means, coupled to said second means, for counting Fourier rows; and (e) fifth means, responsive to said fourth means and coupled to said second and third means, for controlling the calculation of said image such that said time-sequential measurement signals are continuously produced for use by said second means for the calculation of Fourier rows outside a predetermined region of the rows in said matrix, but are intermittently produced for use by said second means as a function of said motion signal when within said region.
Claim 3
Dependent Claim 20 words
The apparatus defined in claim 1, wherein said predetermined row region is preselectable according to the requirements of image quality.
Claim 4
Dependent Claim 19 words
The apparatus defined in claim 1, wherein said predetermined row region comprises approximately 10% of all measured Fourier rows.
Claim 5
Dependent Claim 19 words
The apparatus defined in claim 2, wherein said predetermined row region lies approximately in the center of said matrix.
Claim 6
Dependent Claim 19 words
The apparatus defined in claim 3, wherein said predetermined row region lies approximately in the center of said matrix.
Claim 7
Dependent Claim 270 words
Apparatus for producing images of a test object using nuclear magnetic resonance, at least a portion said test object being subject to physical motion, said apparatus comprising: (a) first means for applying magnetic primary and gradient fields to the test object and for detecting deflection of nuclear spins of the test object from their equilibrium position by a radio-frequency magnetic excitation pulse, said first means producing a plurality of time-sequential measurement signals representative of said nuclear spin deflection in response to a respective plurality of excitation pulses time-sequentially applied with corresponding gradient fields; (b) second means, responsive to said produced measurement signals, for calculating an image of a cross-sectional slice of the test object by Fourier transformation from a matrix of Fourier rows, each Fourier row being calculated from at least one of said time-sequential measurement signals as a projection of the nuclear spins on a frequency axis caused by the plurality of magnetic field gradients in said slice; (c) third means for generating a motion signal representative of said physical motion of of the test object; (d) fourth means, coupled to said second means, for counting Fourier rows; and (e) fifth means, responsive to said fourth means and coupled to said second and third means for controlling the calculation of said image such that said Fourier rows which are outside a predetermined region of rows in said matrix are given a prescribed, synthetic value , but for Fourier rows within said region, selected ones of said measurement signals selected as a function of said motion signal are used by said second means for the calculation of said Fourier rows.
Claim 8
Dependent Claim 270 words
Apparatus for producing images of a test object using nuclear magnetic resonance, at least a portion said test object being subject to physical motion, said apparatus comprising: (a) first means for applying magnetic primary and gradient fields to the test object and for detecting deflection of nuclear spins of the test object from their equilibrium position by a radio-frequency magnetic excitation pulse, said first means producing a plurality of time-sequential measurement signals representative of said nuclear spin deflection in response to a respective plurality of excitation pulses time-sequentially applied with corresponding gradient fields; (b) second means, responsive to said produced measurement signals, for calculating an image of a cross-sectional slice of the test object by Fourier transformation from a matrix of Fourier rows, each Fourier row being calculated from at least one of said time-sequential measurement signals as a projection of the nuclear spins on a frequency axis caused by the plurality of magnetic field gradients in said slice; (c) third means for generating a motion signal representative of said physical motion of of the test object; (d) fourth means, coupled to said second means, for counting Fourier rows; and (e) fifth means, responsive to said fourth means and coupled to said second and third means for controlling the calculation of said image such that said Fourier rows which are outside a predetermined region of rows in said matrix are given a prescribed, synthetic value , but for Fourier rows within said region, selected ones of said measurement signals selected as a function of said motion signal are used by said second means for the calculation of said Fourier rows.
Claim 9
Dependent Claim 20 words
The apparatus defined in claim 6, wherein said predetermined row region is preselectable according to the requirements of image quality.
Claim 10
Dependent Claim 19 words
The apparatus defined in claim 6, wherein said predetermined row region comprises approximately 50% of all measured Fourier rows.
Claim 11
Dependent Claim 19 words
The apparatus defined in claim 7, wherein said predetermined row region lies approximately in the center of said matrix.
Claim 12
Dependent Claim 19 words
The apparatus defined in claim 8, wherein said predetermined row region lies approximately in the center of said matrix.

References Cited (Backward Citations)

DE2854774A1 Cited
US4409550A Cited
US4599565A Cited
US4486708A Cited
EP0093897A1 Cited
EP0096487A1 Cited
US4545384A Cited
US4577152A Cited
US4549140A Cited
US4573014A Cited
US4564017A Cited
US4567893A Cited

USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1990-07-20 1991-01-19 1991-07-21 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 1994-07-20 1995-01-19 1995-07-21 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 1998-07-20 1999-01-19 1999-07-21 $7700.00 Window Closed / Lapsed

Assigned Categories & Tags

No categories assigned to this patent yet.

Assign Category Tag