Apparatus and method for nuclear magnetic resonance scanning and mapping

Claim 5

The method according to claim 2 wherein the field configuration of the primary static magnetic field has a saddle shaped gradient with the region of uniformity at the saddle point and the focusing static magnetic field has an adjustable saddle shaped gradient with the region of uniformity at the saddle point and wherein the size of the resonance domain is adjusted by changing the gradient of the focusing static magnetic field as it approaches its saddle point.

Claim 6

The method according to claim 2 wherein the oscillating magnetic radiation is directed to the resonance domain on a periodic basis and further including the step of repositioning the specimen after a nuclear magnetic resonance signal has been received such that a different portion of the specimen coincides with the resonance domain whereby scanning of the specimen may be accomplished.

Claim 7

The method according to claim 4 wherein the specimen is moved in a planar grid pattern across a cross section of the specimen such that a grid of nuclear magnetic resonance values is obtained for the cross section of the specimen.

Claim 8

The method according to claim 5 further including the step of displaying the grid of nuclear magnetic resonance values to provide a visual image of the grid.

Claim 9

The method according to claim 2 wherein a doughnut shaped superconducting magnet is utilized for providing the primary static magnetic field space and wherein the specimen is positioned within the interior space of the doughnut shaped superconducting magnet.

Claim 10

The method according to claim 7 wherein field focusing coils are used to provide the focusing static magnetic field.

Claim 11

The method according to claim 2 wherein the specimen includes a live mammal and the nuclear magnetic values may include intensitites of nuclear magnetic resonance signals received, spin-spin relaxation time, spin-lattice relaxation times, spin-mapping values, and amplitude versus frequency spectra.

Claim 12

The method according to claim 2 wherein the selected nuclei may be selected from P 31 , K 39 , Na 23 , H 1 , C 13 , N 15 , N 14 or O 17 .

Claim 13

Nuclear magnetic induction apparatus for detecting selected nuclei within a specimen comprising: (a) means for providing a nonuniform primary static magnetic field space; (b) means for focusing the primary static magnetic field space by a time-independent shaping of the primary magnetic field space to provide a three dimensional resonance domain of selectable size wherein the field strength is substantially uniform; (c) means for positioning the specimen such that the resonance domain impinges on the specimen; (d) means for directing oscillating magnetic radiation to the resonance domain such that the magnetic field orientation of the oscillating magnetic radiation is orthogonal to the magnetic field orientation of the primary static magnetic field to cause a nuclear magnetic signal to be generated by selected nuclei within the resonance domain; (e) means for receiving the nuclear magnetic resonance signal generated; and (f) means for processing the nuclear magnetic resonance signal to determine a nuclear magnetic resonance value directly which nuclear magnetic resonance value represents the selected nuclei extant in the resonance domain impinging on the specimen. PG,37

Claim 14

Nuclear magnetic induction apparatus for detecting selected nuclei within a specimen comprising: (a) means for providing a nonuniform primary static magnetic field space; (b) means for focusing the primary static magnetic field space by a time-independent shaping of the primary magnetic field space to provide a three dimensional resonance domain of selectable size wherein the field strength is substantially uniform; (c) means for positioning the specimen such that the resonance domain impinges on the specimen; (d) means for directing oscillating magnetic radiation to the resonance domain such that the magnetic field orientation of the oscillating magnetic radiation is orthogonal to the magnetic field orientation of the primary static magnetic field to cause a nuclear magnetic signal to be generated by selected nuclei within the resonance domain; (e) means for receiving the nuclear magnetic resonance signal generated; and (f) means for processing the nuclear magnetic resonance signal to determine a nuclear magnetic resonance value directly which nuclear magnetic resonance value represents the selected nuclei extant in the resonance domain impinging on the specimen. PG,37

Claim 15

Nuclear magnetic induction apparatus for detecting the selected nuclei within a specimen comprising: (a) means for providing a nonuniform primary static magnetic field having a known field configuration with a region of uniformity where the field strength is substantially uniform; (b) means for providing a time-independent focusing static magnetic field having a selectable field configuration with a region of uniformity where the field strength is substantially uniform; (c) superimposing the time-independent focusing static magnetic field upon the primary static magnetic field such that the respective regions of uniformity coincide to produce a resulting static magnetic field having a three dimensional resonance domain located within a region where the regions of uniformity coincide, the field strength of the resulting static magnetic field within the resonance domain being substantially uniform; (d) means for selecting the field configuration of the time-independent focusing static magnetic field to adjust the size of the resonance domain; (e) means for positioning the specimen such that the resonance domain impinges on the specimen; (f) means for directing oscillating magnetic radiation to the resonance domain such that the magnetic field orientation of the oscillating magnetic radiation is orthogonal to the magnetic field orientation of the resulting magnetic field to cause a nuclear magnetic resonance signal to be generated; (g) receiving the nuclear magnetic signal generated; and (h) processing the signal to determine a nuclear magnetic resonance value directly which nuclear magnetic resonance value represents the selected nuclei extant in the resonance domain within the specimen.

Claim 16

Nuclear magnetic induction apparatus for detecting the selected nuclei within a specimen comprising: (a) means for providing a nonuniform primary static magnetic field having a known field configuration with a region of uniformity where the field strength is substantially uniform; (b) means for providing a time-independent focusing static magnetic field having a selectable field configuration with a region of uniformity where the field strength is substantially uniform; (c) superimposing the time-independent focusing static magnetic field upon the primary static magnetic field such that the respective regions of uniformity coincide to produce a resulting static magnetic field having a three dimensional resonance domain located within a region where the regions of uniformity coincide, the field strength of the resulting static magnetic field within the resonance domain being substantially uniform; (d) means for selecting the field configuration of the time-independent focusing static magnetic field to adjust the size of the resonance domain; (e) means for positioning the specimen such that the resonance domain impinges on the specimen; (f) means for directing oscillating magnetic radiation to the resonance domain such that the magnetic field orientation of the oscillating magnetic radiation is orthogonal to the magnetic field orientation of the resulting magnetic field to cause a nuclear magnetic resonance signal to be generated; (g) receiving the nuclear magnetic signal generated; and (h) processing the signal to determine a nuclear magnetic resonance value directly which nuclear magnetic resonance value represents the selected nuclei extant in the resonance domain within the specimen.

Claim 17

The apparatus according to claim 12 wherein the means for providing oscillating magnetic radiation is actuated on a periodic basis and further includes means for repositioning the specimen with respect to the resonance domain after a nuclear magnetic resonance signal has been received such that a different portion of the specimen coincides with the resonance domain whereby scanning of the specimen may be accomplished.

Claim 18

The apparatus according to claim 12 wherein the means for providing a primary static magnetic field comprises a doughnut shaped superconducting magnet.

Claim 19

The apparatus according to claim 12 wherein the means for providing a focusing static magnetic field comprises field focusing coils.