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EP0154996A2 Expired / Lapsed EP ⏱️ 0.0 years remaining

Magnetic resonance imaging apparatus using shim coil correction

Assignee: Toshiba Corp
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Filing: 1985-03-13
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Granted: —
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Expires: 2005-03-13
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Abstract

Abstract In an NMR imaging apparatus (100), the steady magnetic field (H o ) is subjected to be deformed. The first shim coil pair (20) is wound on a common bobbin (40) and has a common diameter (2a). The second shim coil pair (30) is wound on the same bobbin (40) and has the same diameter (2a) as that of the first shim coil pair (20). The first shim coil pair (20) corrects homogeneity of the field components of the steady magnetic field (H o ) having even-numbered higher order terms in the longitudinal axis (Z) of the object (P) under examination. The second shim coil pair (30) corrects uniformity of the magnetic field components of the steady magnetic field (H o ) in the direction (R) perpendicular to the longitudinal axis (Z) and also uniformity of the magnetic field components of the first coil pair (20) in the direction (R) perpendicular to the longitudinal axis (Z).

Inventors

  • 👤 Hiroshi C/O Patent Division Sugimoto

Bibliographic Details

Application Number —
Jurisdiction EP
Data Source google_patents
Last Synchronized 2026-11-08 15:05
CPC Classifications
G; G01; G01R; G01R33/00; G01R33/20; G01R33/28; G01R33/38; G01R33/387; G01R33/3875

Claims Analysis

Total Claims: 8
Claim 1
Independent Claim 450 words
An imaging apparatus (100) for examining an object (P) having a longitudinal axis (Z) and a cross-sectional slice (S) perpendicular thereto, by nuclear magnetic resonance, characterized by comprising: magnetic means (1;2) for applying to said object (P) a steady magnetic field (H o ) along said longitudinal axis (Z); first coil means (3;4), which is arranged along said longitudinal axis (Z), for applying to said object (P) a first gradient field (G z ), which in conjunction with said steady magnetic field (H o ) provides a predetermined field in said cross-sectional slice (S) of said object (P), the field direction of said first gradient field (G z ) being parallel to that of said steady magnetic field (H o ) and the absolute value of the field strength value of said first gradient field (G z ) increasing linearly in opposite directions from said cross-sectional slice along said longitudinal axis; probe head coil means (6) for applying RF pulses to said cross-sectional slice (S) in a direction perpendicular to said longitudinal axis (Z) so as to excite nuclei therein which are being subjected to said predetermined field, and for detecting nuclear magnetic resonance signals derived from said cross-sectional slice (S); second coil means (3;4) for applying a second gradient field (G x ;Gy) to said cross-sectional slice (S) so as to define a projection angle of said nuclear magnetic resonance signals, the field direction of said second gradient field (G x ;Gy) being perpendicular to said steady magnetic field (H o ) and the strength of said second gradient field (G x ;Gy) varying linearly, orthogonal to said first gradient field (G z ); signal processing means (8) for receiving said nuclear magnetic resonance signals from said probe head means (6), and for processing said received nuclear magnetic resonance signals by use of a two-dimensional Fourier transformation to produce an image of said cross-sectional slice (S); and, correction coil means (10;12;14) having at least first and second coil pairs (20;30;60), said first coil pair (20;30) generating in conjunction with said steady magnetic field (H o ) a first correction magnetic field so as to correct homogeneity of magnetic field components of said steady magnetic field (H o ) having even-numbered higher order terms in said longitudinal axis (Z), and said second coil pair (30;60) generating in conjunction with said steady magnetic field (H o ) a second correction magnetic field so as to correct uniformity of magnetic field components of said steady magnetic field (H o ) in a direction (R) perpendicular to said longitudinal axis (Z), and also uniformity of magnetic field components of said first coil pair in said direction (R) perpendicular to said longitudinal axis (Z).
Claim 2
Dependent Claim 450 words
An imaging apparatus (100) for examining an object (P) having a longitudinal axis (Z) and a cross-sectional slice (S) perpendicular thereto, by nuclear magnetic resonance, characterized by comprising: magnetic means (1;2) for applying to said object (P) a steady magnetic field (H o ) along said longitudinal axis (Z); first coil means (3;4), which is arranged along said longitudinal axis (Z), for applying to said object (P) a first gradient field (G z ), which in conjunction with said steady magnetic field (H o ) provides a predetermined field in said cross-sectional slice (S) of said object (P), the field direction of said first gradient field (G z ) being parallel to that of said steady magnetic field (H o ) and the absolute value of the field strength value of said first gradient field (G z ) increasing linearly in opposite directions from said cross-sectional slice along said longitudinal axis; probe head coil means (6) for applying RF pulses to said cross-sectional slice (S) in a direction perpendicular to said longitudinal axis (Z) so as to excite nuclei therein which are being subjected to said predetermined field, and for detecting nuclear magnetic resonance signals derived from said cross-sectional slice (S); second coil means (3;4) for applying a second gradient field (G x ;Gy) to said cross-sectional slice (S) so as to define a projection angle of said nuclear magnetic resonance signals, the field direction of said second gradient field (G x ;Gy) being perpendicular to said steady magnetic field (H o ) and the strength of said second gradient field (G x ;Gy) varying linearly, orthogonal to said first gradient field (G z ); signal processing means (8) for receiving said nuclear magnetic resonance signals from said probe head means (6), and for processing said received nuclear magnetic resonance signals by use of a two-dimensional Fourier transformation to produce an image of said cross-sectional slice (S); and, correction coil means (10;12;14) having at least first and second coil pairs (20;30;60), said first coil pair (20;30) generating in conjunction with said steady magnetic field (H o ) a first correction magnetic field so as to correct homogeneity of magnetic field components of said steady magnetic field (H o ) having even-numbered higher order terms in said longitudinal axis (Z), and said second coil pair (30;60) generating in conjunction with said steady magnetic field (H o ) a second correction magnetic field so as to correct uniformity of magnetic field components of said steady magnetic field (H o ) in a direction (R) perpendicular to said longitudinal axis (Z), and also uniformity of magnetic field components of said first coil pair in said direction (R) perpendicular to said longitudinal axis (Z).
Claim 3
Dependent Claim 23 words
An apparatus (100) as claimed in Claim 1, characterized in that said even-numbered higher order terms are selected to be two order terms.
Claim 4
Dependent Claim 57 words
An apparatus (100) as claimed in Claim 1, characterized in that each of said first and second coil pairs has first and second coil halves (10A;10B:10C;10D) having a common diameter, and a given ratio (b/a) of a distance "2b" to said common diameter "2a", said distance being measured between the respective first and second coil halves (10A;10B:10C;10D).
Claim 5
Dependent Claim 70 words
An apparatus (100) as claimed in claim 3, characterized in that said ratio (bl/a) of said first coil pair (20) is set to be 0.30 and said ratio (b2/a) of said second coil pair (30) is set to be 0.62, while first and second currents (ilOA;ilOB:ilOC;ilOD) flowing through said first and second coil pairs (20;30) are 1 ampere respectively and the turn numbers thereof are commonly selected to be 1.
Claim 6
Dependent Claim 77 words
An apparatus (100) as claimed in Claim 3, characterized in that said ratio (b3/a) of said first coil pair (60) is selected to be 1.18 and said ratio (b2/a) of said second coil pair (30) is selected to be 0.62, while first current (ilOE;ilOF) of said first coil pair (60) is - 0.231 ampere, second current (ilOC;ilOD) of said second coil pair (30) is 1 ampere, and the turn numbers thereof are commonly selected to be 1.
Claim 7
Dependent Claim 50 words
An apparatus (100) as claimed in claim 3, characterized by further comprising a third coil pair (60) having first and second coil halves (10E;10F) and a given ratio (b3/a) of a third distance "2b3" to a third diameter "2a3" said third distance being measured between said respective coil halves (10E;10F).
Claim 8
Dependent Claim 102 words
An apparatus (100) as claimed in claim 6, characterized in that said ratio (bl/a) of said first coil pair (20) is selected to be 0.30, said ratio (b2/a) of said second coil pair (30) is set to be 0.62, and said ratio (b3/a) of said third coil pair (60) is chosen to be 1.18, while first current (ilOA;ilOB) of said first coil pair (20) is 1 ampere, second current (ilOC;ilOD) of said second coil pair (30) is - 0.231 ampere, third current (ilOE;ilOF) of said third coil pair (60) is 0.769 ampere, and turn numbers thereof are commonly selected to be 1.

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