Pulsed field MRI system with non-resonant excitation

Claim 2

In a method for imaging an object using magnetic resonance without radio-frequency excitation the steps of: applying a magnetic pulse through the object producing a distribution of magnetic moments in a first direction; applying a plurality of orthogonal magnetic gradients through the object whose magnetic field points substantially normal to the first direction; receiving signals, following the magnetic pulse, resulting from the precessing magnetic moments in the object normal to the gradient field; and processing the received signals to form an image representing the magnetic moment distribution in the object.

Claim 3

The method as described in claim 1 where the step of applying the magnetic pulse includes the steps of: increasing the magnetic field from zero to a maximum value; decreasing the magnetic field from the maximum value down to a value substantially higher than the magnetic field orthogonal to the magnetic pulse field; and further decreasing the magnetic field at a rate greater than the adiabatic condition whereby the magnetic moments will remain pointing substantially in the direction of the pulsed field.

Claim 4

The method as described in claim 2 where the step of decreasing the magnetic field includes the step of decreasing the magnetic field from the maximum value to a value substantially higher than the magnetic field orthogonal to the magnetic pulse field at a rate which satisfies the adiabatic condition whereby the magnetic moments point to the resultant magnetic field.

Claim 5

The method as described in claim 1 where the step of applying a magnetic pulse includes the step of controlling the duration of the pulse to be a fraction of the T 1 relaxation time whereby the resultant received signals will be dependent on T 1 .

Claim 6

The method as described in claim 1 where the step of applying a plurality of orthogonal magnetic gradients includes the step of starting at least one gradient before the magnetic pulse ends whereby the required gradient bandwidth is reduced.

Claim 7

The method as described in claim 1 including the step of adding a constant magnetic field in the same direction as the gradient field whose amplitude is greater than the strongest field due to the gradients whereby the resultant field substantially normal to the first direction will not change polarity.

Claim 8

The method as described in claim 1 where the step of applying gradients includes the step of applying three spatially orthogonal gradient fields and the step of repeating the entire sequence while varying the gradient fields so as to span the three dimensional spatial transform of the object.

Claim 9

The method as described in claim 1 where the step of applying gradients includes the step of applying two spatially orthogonal gradient fields and the step of repeating the entire sequence while varying the gradient fields so as to span the two dimensional spatial transform of a two-dimensional projection of the object.

Claim 10

The method as described in claim 1 where the step of applying spatially orthogonal gradients includes the step of applying an oscillating gradient to one spatial axis.

Claim 11

The method as described in claim 9 where the step of applying a magnetic pulse includes the step of terminating the pulse during a time interval where the oscillating gradient is substantially zero.

Claim 12

The method as described in claim 1 where the step of applying spatially orthogonal gradients includes the step of applying constant fields to two of the gradients whereby a radial line is traced in the k-space of the object of those two dimensions.

Claim 13

The method as described in claim 1 where the step of applying spatially orthogonal gradients includes the step of applying temporally orthogonal growing oscillatory waveforms to two of the gradients whereby a spiral is traced in the k-space of the object of those two dimensions.

Claim 14

The method as described in claim 1 where the step of applying spatially orthogonal gradients includes the step of applying waveforms which coarsely scan the k-space of the object and the step of applying gradient waveforms on subsequent scans which are interleaved with the first scan whereby all of k-space is covered in a plurality of scans.

Claim 15

The method as described in claim 1 where the step of applying a plurality of gradients includes the step of delaying the onset of the gradients following the magnetic pulse whereby the resultant image is dependent on the T 2 relaxation time.

Claim 16

The method as described in claim 1 where the step of applying a plurality of gradients includes the step of applying one gradient waveform which reaches its zero area time, or gradient echo time, delayed from the magnetic pulse whereby the resultant image is dependent on the T 2 relaxation time.

Claim 17

The method as described in claim 1 where the step of receiving signals includes the step of detecting the magnetic field resulting from the magnetic precessing moments in the object normal to the gradient field.

Claim 18

The method as described in claim 16 where the detecting step includes the step of detecting the derivative of the magnetic field using a coil whose axis is substantially normal to the axis of the precessing moments.

Claim 19

The method as described in claim 16 where the detecting step includes the step of detecting the magnetic field in two directions both normal to the gradient field and normal to each other.

Claim 20

The method as described in claim 1 where the step of applying gradients includes the step of applying gradient waveforms which have a net zero area whereby the magnetic moments will all be pointed in the same direction prior to the next pulse.

Claim 21

The method as described in claim 1 where the step of applying a magnetic pulse includes the steps of charging a capacitor and connecting the capacitor to a coil which produces the pulsed field as a half sinusoid.

Claim 22

The method as described in claim 20 including the step of reducing the capacitor size during the decaying portion of the pulse whereby the rate of decay is increased.

Claim 23

The method as described in claim 1 including the step of applying a constant magnetic field substantially normal to the direction of the pulsed field and the where the step of applying a magnetic pulse includes the step of adiabatically decreasing the magnetic field whereby the magnetic moments in the object point in the direction of the constant field and precess about the gradient field substantially normal to the constant field.

Claim 24

In a method for imaging an object using magnetic resonance the steps of: applying a magnetic pulse through the object in a first direction producing a distribution of magnetic moments pointed in the first direction; applying a second magnetic field, substantially smaller than the amplitude of the pulsed field, normal to the direction of the pulsed field causing the magnetic moments to precess normal to the second field; applying radio frequency excitation normal to the second field at a frequency substantially equal to the product of the gyromagnetic radio times the amplitude of the second field along with a magnetic gradient whose field points in the same direction as the second field whereby only a selected portion of the object has precessing magnetic moments; applying a plurality of orthogonal magnetic gradients through the object, following the radio frequency excitation, whose magnetic field points normal to the field of the magnetic pulse; receiving signals, following the radio frequency excitation, resulting from the precessing magnetic moments in the object normal to the gradient field; and processing the received signals to form an image representing the magnetic moment distribution in the object.

Claim 25

In a method for imaging an object using magnetic resonance the steps of: applying a magnetic pulse through the object in a first direction producing a distribution of magnetic moments pointed in the first direction; applying a second magnetic field, substantially smaller than the amplitude of the pulsed field, normal to the direction of the pulsed field causing the magnetic moments to precess normal to the second field; applying radio frequency excitation normal to the second field at a frequency substantially equal to the product of the gyromagnetic radio times the amplitude of the second field along with a magnetic gradient whose field points in the same direction as the second field whereby only a selected portion of the object has precessing magnetic moments; applying a plurality of orthogonal magnetic gradients through the object, following the radio frequency excitation, whose magnetic field points normal to the field of the magnetic pulse; receiving signals, following the radio frequency excitation, resulting from the precessing magnetic moments in the object normal to the gradient field; and processing the received signals to form an image representing the magnetic moment distribution in the object.

Claim 26

The method as described in claim 23 where the step of applying the radio frequency excitation along with the gradient includes the step of selectively removing the moments from all portions of the object except the selected portion.

Claim 27

The method as described in claim 23 where the step of applying the radio frequency excitation along with the gradient includes the step of rotating all of the magnetic moments in the object into the direction of the second field and selectively rotating the magnetic moments in the selected portion of the object normal to the second field whereby they precess and produce signals.

Claim 28

Apparatus for imaging an object using magnetic resonance without radio-frequency excitation comprising: means for applying a magnetic pulse through the object producing a distribution of magnetic moments in a first direction; means for applying a plurality of orthogonal magnetic gradients through the object whose magnetic field points substantially normal to the first direction; means for receiving signals, following the magnetic pulse, resulting from the precessing magnetic moments in the object normal to the gradient field; and means for processing the received signals to form an image representing the magnetic moment distribution in the object.

Claim 29

Apparatus for imaging an object using magnetic resonance without radio-frequency excitation comprising: means for applying a magnetic pulse through the object producing a distribution of magnetic moments in a first direction; means for applying a plurality of orthogonal magnetic gradients through the object whose magnetic field points substantially normal to the first direction; means for receiving signals, following the magnetic pulse, resulting from the precessing magnetic moments in the object normal to the gradient field; and means for processing the received signals to form an image representing the magnetic moment distribution in the object.

Claim 30

Apparatus as described in claim 26 where the means for applying the magnetic pulse includes: means for increasing the magnetic field from zero to a maximum value; means for decreasing the magnetic field from the maximum value down to a value substantially higher than the magnetic field orthogonal to the magnetic pulse field; and means for furthur decreasing the magnetic field at a rate greater than the adiabatic condition whereby the magnetic moments will remain pointing substantially in the direction of the pulsed field.

Claim 31

Apparatus as described in claim 27 where the means for decreasing the magnetic field includes the means for decreasing the magnetic field from the maximum value to a value substantially higher than the magnetic field orthogonal to the magnetic pulse field at a rate which satisfies the adiabatic condition whereby the magnetic moments point to the resultant magnetic field.

Claim 32

Apparatus as described in claim 26 where the means for applying a magnetic pulse includes means for controlling the duration of the pulse to be a fraction of the T 1 relaxation time whereby the resultant received signals will be dependent on T 1 .

Claim 33

Apparatus as described in claim 26 where the means for applying a plurality of orthogonal magnetic gradients includes means for starting at least one gradient before the magnetic pulse ends whereby the required gradient bandwidth is reduced.

Claim 34

Apparatus as described in claim 26 including means for adding a constant magnetic field in the same direction as the gradient field whose amplitude is greater than the strongest field due to the gradients whereby the resultant field normal to the pulsed field will not change polarity.

Claim 35

Apparatus as described in claim 26 where the means for applying gradients includes means for applying three spatially orthogonal gradient fields and means for repeating the entire sequence while varying the gradient fields so as to span the three dimensional spatial transform of the object.

Claim 36

Apparatus as described in claim 26 where the means for applying gradients includes means for applying two spatially orthogonal gradient fields and means for repeating the entire sequence while varying the gradient fields so as to span the two dimensional spatial transform of a two-dimensional projection of the object.

Claim 37

Apparatus as described in claim 26 where the means for applying spatially orthogonal gradients includes means for applying an oscillating gradient to one spatial axis.

Claim 38

Apparatus as described in claim 34 where the means for applying a magnetic pulse includes means for terminating the pulse during a time interval where the oscillating gradient is substantially zero.

Claim 39

Apparatus as described in claim 26 where the means for applying spatially orthogonal gradients includes means for applying constant fields to two of the gradients whereby a radial line is traced in the k-space of those two dimensions.

Claim 40

Apparatus as described in claim 26 where the means for applying spatially orthogonal gradients includes means for applying oscillatory increasing-amplitude temporally orthogonal waveforms to two of the gradients whereby a spiral is traced in the k-space of these two dimensions.

Claim 41

Apparatus as described in claim 26 where the means for applying spatially orthogonal gradients includes means for applying waveforms which coarsely scan k-space and means for applying waveforms on subsequent scans which are interleaved with the first scan whereby all of k-space is substantially covered in a plurality of scans.

Claim 42

Apparatus as described in claim 26 where the means for applying a plurality of gradients includes means for delaying the onset of the gradients following the magnetic pulse whereby the resultant image is dependent on the T 2 relaxation time.

Claim 43

Apparatus as described in claim 26 where the means for applying a plurality of gradients includes means for applying one gradient waveform which reaches its zero area time, or gradient echo time, delayed from the magnetic pulse whereby the resultant image is dependent on the T 2 relaxation time.

Claim 44

Apparatus as described in claim 26 where the means for receiving signals includes means for detecting the magnetic field resulting from the precessing magnetic moments in the object normal to the gradient field.

Claim 45

Apparatus as described in claim 41 where the detecting means includes means for detecting the derivative of the magnetic field using a coil whose axis is substantially normal to the axis of the precessing moments.

Claim 46

Apparatus as described in claim 41 where the detecting means includes the means for detecting the magnetic field in two directions both substantially normal to the gradient field and substantially normal to each other.

Claim 47

Apparatus as described in claim 26 where the means for applying gradients includes means for applying gradient waveforms which have a net zero area whereby the magnetic moments will all be pointed in the same direction prior to the application of the next magnetic pulse.

Claim 48

Apparatus as described in claim 44 including means for applying a magnetic pulse in the direction of the gradient field whereby the direction of the magnetic moments is altered.

Claim 49

Apparatus as described in claim 26 where the means for applying a magnetic pulse includes means for charging a capacitor and connecting the capacitor to a coil which produces the pulsed field as a half sinusoid.

Claim 50

Apparatus as described in claim 46 including the means for reducing the capacitor size during the decaying portion of the pulse whereby the rate of decay is increased.

Claim 51

Apparatus as described in claim 26 including means for applying a constant magnetic field substantially normal to the direction of the pulsed field and where the means for applying a pulsed magnetic field includes means for adiabatically decreasing the field amplitude whereby the magnetic moments will point in the direction of the constant field and precess about the gradient field substantially normal to the constant field.

Claim 52

Apparatus for imaging an object using magnetic resonance comprising: means for applying a magnetic pulse through the object in a first direction producing a distribution of magnetic moments pointing in the first direction; means for applying a second magnetic field, substantially smaller than the amplitude of the pulsed field, normal to the direction of the pulsed field causing the magnetic moments to precess normal to the second field; means for applying radio frequency excitation normal to the second field at a frequency substantially equal to the product of the gyromagnetic ratio times the amplitude of the second field along with a magnetic gradient whose field points in the same direction as the second field whereby only a selected portion of the object has precessing magnetic moments; means for applying a plurality of orthogonal magnetic gradients through the object, following the radio frequency excitation, whose magnetic field points normal to the field of the magnetic pulse; means for receiving signals, following the radio frequency excitation, resulting from the precessing magnetic moments in the object normal to the gradient field; and means for processing the received signals to form an image representing the magnetic moment distribution in the object.

Claim 53

Apparatus for imaging an object using magnetic resonance comprising: means for applying a magnetic pulse through the object in a first direction producing a distribution of magnetic moments pointing in the first direction; means for applying a second magnetic field, substantially smaller than the amplitude of the pulsed field, normal to the direction of the pulsed field causing the magnetic moments to precess normal to the second field; means for applying radio frequency excitation normal to the second field at a frequency substantially equal to the product of the gyromagnetic ratio times the amplitude of the second field along with a magnetic gradient whose field points in the same direction as the second field whereby only a selected portion of the object has precessing magnetic moments; means for applying a plurality of orthogonal magnetic gradients through the object, following the radio frequency excitation, whose magnetic field points normal to the field of the magnetic pulse; means for receiving signals, following the radio frequency excitation, resulting from the precessing magnetic moments in the object normal to the gradient field; and means for processing the received signals to form an image representing the magnetic moment distribution in the object.

Claim 54

Apparatus as described in claim 49 where the means for applying the radio frequency excitation along with the gradient includes means for selectively removing the moments from all portions of the object except the selected portion.

Claim 55

Apparatus as described in claim 49 where the means for applying the radio frequency excitation along with the gradient includes means for rotating all of the magnetic moments in the object into the direction of the second field and selectively rotating the magnetic moments in the selected portion of the object normal to the second field whereby they precess and produce signals.

Claim 56

In a method for imaging an object using magnetic resonance the steps of: applying a magnetic pulse through the object in a first direction; applying a smaller magnetic field normal to the first direction which is turned on prior to the end of the magnetic pulse; controlling the rate of decay of the magnetic pulse so that the magnetic moments point in the direction of the smaller magnetic field at the end of the pulse; applying radio frequency excitation normal to the smaller field at a frequency substantially equal to the product of the gyromagnetic ratio times the amplitude of the smaller field along with a magnetic gradient whose field points in the same direction as the smaller field whereby a selected portion of the object has precessing magnetic moments normal to the smaller field; applying a plurality of orthogonal magnetic gradients through the object, following the radio frequency excitation, whose magnetic field points in the direction of the smaller field; receiving signals, following the radio frequency excitation, resulting from the precessing magnetic moments in the object normal to the gradient field; and processing the received signals to form an image representing the magnetic moment distribution in the object.

Claim 57

In a method for imaging an object using magnetic resonance the steps of: applying a magnetic pulse through the object in a first direction; applying a smaller magnetic field normal to the first direction which is turned on prior to the end of the magnetic pulse; controlling the rate of decay of the magnetic pulse so that the magnetic moments point in the direction of the smaller magnetic field at the end of the pulse; applying radio frequency excitation normal to the smaller field at a frequency substantially equal to the product of the gyromagnetic ratio times the amplitude of the smaller field along with a magnetic gradient whose field points in the same direction as the smaller field whereby a selected portion of the object has precessing magnetic moments normal to the smaller field; applying a plurality of orthogonal magnetic gradients through the object, following the radio frequency excitation, whose magnetic field points in the direction of the smaller field; receiving signals, following the radio frequency excitation, resulting from the precessing magnetic moments in the object normal to the gradient field; and processing the received signals to form an image representing the magnetic moment distribution in the object.

Claim 58

Apparatus for imaging an object using magnetic resonance comprising: means for applying a magnetic pulse through the object in a first direction; means for applying a smaller magnetic field normal to the first direction which is turned on prior to the end of the magnetic pulse; means for controlling the rate of decay of the magnetic pulse so that the magnetic moments point in the direction of the smaller magnetic field at the end of the pulse; means for applying radio frequency excitation normal to the smaller field at a frequency substantially equal to the product of the gyromagnetic ratio times the amplitude of the smaller field along with a magnetic gradient whose field points in the same direction as the smaller field whereby a selected portion of the object has precessing magnetic moments normal to the smaller field; means for applying a plurality of orthogonal magnetic gradients through the object, following the radio frequency excitation, whose magnetic field points in the direction of the smaller field; means for receiving signals, following the radio frequency excitation, resulting from the precessing magnetic moments in the object normal to the gradient field; and means for processing the received signals to form an image representing the magnetic moment distribution in the object.

Claim 59

Apparatus for imaging an object using magnetic resonance comprising: means for applying a magnetic pulse through the object in a first direction; means for applying a smaller magnetic field normal to the first direction which is turned on prior to the end of the magnetic pulse; means for controlling the rate of decay of the magnetic pulse so that the magnetic moments point in the direction of the smaller magnetic field at the end of the pulse; means for applying radio frequency excitation normal to the smaller field at a frequency substantially equal to the product of the gyromagnetic ratio times the amplitude of the smaller field along with a magnetic gradient whose field points in the same direction as the smaller field whereby a selected portion of the object has precessing magnetic moments normal to the smaller field; means for applying a plurality of orthogonal magnetic gradients through the object, following the radio frequency excitation, whose magnetic field points in the direction of the smaller field; means for receiving signals, following the radio frequency excitation, resulting from the precessing magnetic moments in the object normal to the gradient field; and means for processing the received signals to form an image representing the magnetic moment distribution in the object.

Claim 60

In a method for imaging flowing material in a selected portion of an object the steps of: applying a pulsed magnetic field to a source of flowing material in the object to form magnetic moments; applying a set of orthogonal gradients to the selected portion whose field is substantially normal to the magnetic gradients whereby the moments precess; receiving signals from the precessing magnetic moments which have flowed from the source of flowing material to the selected portion of the object; and processing the received signals to form an image of the flowing material.

Claim 61

In a method for imaging flowing material in a selected portion of an object the steps of: applying a pulsed magnetic field to a source of flowing material in the object to form magnetic moments; applying a set of orthogonal gradients to the selected portion whose field is substantially normal to the magnetic gradients whereby the moments precess; receiving signals from the precessing magnetic moments which have flowed from the source of flowing material to the selected portion of the object; and processing the received signals to form an image of the flowing material.

Claim 62

The method as described in claim 54 where the step of applying a pulsed magnetic field to a source of flowing material includes the step of applying a static magnetic field to the source of flowing material whereby the flowing material experiences a pulsed field.