Nuclear magnetic resonance systems

Claim 1

A method of examining a slice of a body of nuclear magnetic resonance, said method comprising the steps of: (a) applying to the body a steady magnetic field along an axis therein; (b) applying a first gradient magnetic field which, in conjunction with the steady field, gives a predetermined magnetic field in said slice of the body; (c) in conjunction with the first gradient field, applying a periodic magnetic field at the Larmor frequency for the predetermined field in the slice to cause resonance therein, and (d) subsequently sensing resonance signals in the presence of a further gradient magnetic field and using said resonance signals to evaluate said slice, wherein the periodic field is applied in first and second distinct pulses, each in conjunction with said first gradient field, the total field integral of the periodic field being sufficient to rotate the spin vectors of nuclei in the slice through an angle of π/2 radians and between the first and second pulses there is applied a further pulse of the periodic field applied in the absence of the first gradient magnetic field, of field integral sufficient to rotate the spin vectors through an angle of π radians.

Claim 2

A method of examining a slice of a body of nuclear magnetic resonance, said method comprising the steps of: (a) applying to the body a steady magnetic field along an axis therein; (b) applying a first gradient magnetic field which, in conjunction with the steady field, gives a predetermined magnetic field in said slice of the body; (c) in conjunction with the first gradient field, applying a periodic magnetic field at the Larmor frequency for the predetermined field in the slice to cause resonance therein, and (d) subsequently sensing resonance signals in the presence of a further gradient magnetic field and using said resonance signals to evaluate said slice, wherein the periodic field is applied in first and second distinct pulses, each in conjunction with said first gradient field, the total field integral of the periodic field being sufficient to rotate the spin vectors of nuclei in the slice through an angle of π/2 radians and between the first and second pulses there is applied a further pulse of the periodic field applied in the absence of the first gradient magnetic field, of field integral sufficient to rotate the spin vectors through an angle of π radians.

Claim 6

A method of examining a slice of a body by nuclear magnetic resonance, said method comprising the steps of: (a) applying to the body a steady magnetic field along an axis therein; (b) applying a first gradient magnetic field which, in conjunction with the steady field, gives a predetermined magnetic field in said slice of the body; (c) in conjunction with the first gradient field, applying a periodic magnetic field at the Larmor frequency for the predetermined field in the slice to cause resonance therein; (d) subsequently sensing resonance signals in the presence of a second gradient magnetic field and using said resonance signals to evaluate said slice, wherein the periodic field is applied in first and second distinct pulses, each in conjunction with said first gradient field, the total field integral of the periodic field being sufficient to rotate the spin vectors of nuclei in the slice through a desired angle and between the first and second pulses there is applied a further pulse of the periodic field applied in the absence of the first gradient magnetic field, of a field integral sufficient to rotate the spin vectors through an angle of π radians.

Claim 7

A method of examining a slice of a body by nuclear magnetic resonance, said method comprising the steps of: (a) applying to the body a steady magnetic field along an axis therein; (b) applying a first gradient magnetic field which, in conjunction with the steady field, gives a predetermined magnetic field in said slice of the body; (c) in conjunction with the first gradient field, applying a periodic magnetic field at the Larmor frequency for the predetermined field in the slice to cause resonance therein; (d) subsequently sensing resonance signals in the presence of a second gradient magnetic field and using said resonance signals to evaluate said slice, wherein the periodic field is applied in first and second distinct pulses, each in conjunction with said first gradient field, the total field integral of the periodic field being sufficient to rotate the spin vectors of nuclei in the slice through a desired angle and between the first and second pulses there is applied a further pulse of the periodic field applied in the absence of the first gradient magnetic field, of a field integral sufficient to rotate the spin vectors through an angle of π radians.

Claim 8

A method of examining a slice of a body by nuclear magnetic resonance, said method comprising the steps of: (a) applying to the body a steady magnetic field along an axis therein; (b) applying a first gradient magnetic field which, in conjunction with the steady field, gives a predetermined magnetic field in said slice of body; (c) in conjunction with the first gradient field, applying a periodic magnetic field at the Larmor frequency for the predetermined field in the slice to cause resonance therein, said periodic field being applied in first and second distinct pulses, each in conjunction with said first gradient field, the total field integral of the periodic field being sufficient to rotate the spin vectors of nuclei in the slice through a desired angle; (d) applying, between said first and second pulses an intermediate pulse of the periodic field, while temporarily removing the first gradient magnetic field, said intermediate pulse being of field integral sufficient to rotate the spin vectors through an angle of π radians; (e) producing a second gradient magnetic field; (f) producing resonance indicating signals during application of said second gradient magnetic field, and (g) utilizing said resonance indicating signals to evaluate said slice.

Claim 9

A method of examining a slice of a body by nuclear magnetic resonance, said method comprising the steps of: (a) applying to the body a steady magnetic field along an axis therein; (b) applying a first gradient magnetic field which, in conjunction with the steady field, gives a predetermined magnetic field in said slice of body; (c) in conjunction with the first gradient field, applying a periodic magnetic field at the Larmor frequency for the predetermined field in the slice to cause resonance therein, said periodic field being applied in first and second distinct pulses, each in conjunction with said first gradient field, the total field integral of the periodic field being sufficient to rotate the spin vectors of nuclei in the slice through a desired angle; (d) applying, between said first and second pulses an intermediate pulse of the periodic field, while temporarily removing the first gradient magnetic field, said intermediate pulse being of field integral sufficient to rotate the spin vectors through an angle of π radians; (e) producing a second gradient magnetic field; (f) producing resonance indicating signals during application of said second gradient magnetic field, and (g) utilizing said resonance indicating signals to evaluate said slice.

Claim 10

A system for examining a slice of a body by use of nuclear magnetic resonance, said system comprising: (a) a first source for applying to the body a steady magnetic field along an axis therein; (b) a second source for applying a first gradient magnetic field which, in conjunction with said steady field, gives a predetermined magnetic field in said slice of the body; (c) a third source for applying, in conjunction with the first gradient field, a periodic magnetic field at the Larmor frequency for the predetermined field in the slice to cause resonance therein; (d) means for subsequently sensing resonance signals in the presence of a second gradient magnetic field and utilizing said resonance signals to evaluate the slice, said periodic field being applied in first and second discrete pulses, each in conjunction with said first gradient field, the total field integral of the periodic field being sufficient to rotate the spin vectors of nuclei in slice through a desired angle and between the first and second pulses there is applied a further pulse of the periodic field applied in the absence of the first gradient magnetic field, of a field integral sufficient to rotate the spin vectors through an angle π radians.

Claim 11

A system for examining a slice of a body by use of nuclear magnetic resonance, said system comprising: (a) a first source for applying to the body a steady magnetic field along an axis therein; (b) a second source for applying a first gradient magnetic field which, in conjunction with said steady field, gives a predetermined magnetic field in said slice of the body; (c) a third source for applying, in conjunction with the first gradient field, a periodic magnetic field at the Larmor frequency for the predetermined field in the slice to cause resonance therein; (d) means for subsequently sensing resonance signals in the presence of a second gradient magnetic field and utilizing said resonance signals to evaluate the slice, said periodic field being applied in first and second discrete pulses, each in conjunction with said first gradient field, the total field integral of the periodic field being sufficient to rotate the spin vectors of nuclei in slice through a desired angle and between the first and second pulses there is applied a further pulse of the periodic field applied in the absence of the first gradient magnetic field, of a field integral sufficient to rotate the spin vectors through an angle π radians.

Claim 12

A system for examining a slice of a body by nuclear magnetic resonance, said system comprising: (a) a first source for applying to the body a steady magnetic field along an axis therein; (b) means for applying a first gradient magnetic field which, in conjunction with the steady field, produces a predetermined magnetic field in said slice of the body; (c) a source for producing, in conjunction with the first gradient field, a periodic field at the Larmor frequency for said predetermined field in the slice to cause resonance within the slice, said periodic field source applying said periodic field in first and second discrete pulses, each pulse in conjunction with said first gradient field, the total field integral of the periodic field being sufficient to rotate the spin vectors of nuclei in the slice through a desired angle; (d) means associated with said periodic field source for applying, between said first and second periodic field pulses, an intermediate pulse of the periodic field, while temporarily removing the first gradient magnetic field, said intermediate pulse being of field integral sufficient to rotate the spin vectors through an angle of π radians; (e) means for producing a second gradient magnetic field; (f) a detector for producing resonance indicating signals during application of said second gradient magnetic field, and (g) interpretive means for utilizing said resonance indicating signals to evaluate a characteristic of said slice.

Claim 13

A system for examining a slice of a body by nuclear magnetic resonance, said system comprising: (a) a first source for applying to the body a steady magnetic field along an axis therein; (b) means for applying a first gradient magnetic field which, in conjunction with the steady field, produces a predetermined magnetic field in said slice of the body; (c) a source for producing, in conjunction with the first gradient field, a periodic field at the Larmor frequency for said predetermined field in the slice to cause resonance within the slice, said periodic field source applying said periodic field in first and second discrete pulses, each pulse in conjunction with said first gradient field, the total field integral of the periodic field being sufficient to rotate the spin vectors of nuclei in the slice through a desired angle; (d) means associated with said periodic field source for applying, between said first and second periodic field pulses, an intermediate pulse of the periodic field, while temporarily removing the first gradient magnetic field, said intermediate pulse being of field integral sufficient to rotate the spin vectors through an angle of π radians; (e) means for producing a second gradient magnetic field; (f) a detector for producing resonance indicating signals during application of said second gradient magnetic field, and (g) interpretive means for utilizing said resonance indicating signals to evaluate a characteristic of said slice.