MRI imaging system using a periodic bias field

Claim 2

In a method for imaging the magnetic spin density in an object the steps of: polarizing the magnetic moments in the object; applying gradient fields and a substantially spatially uniform cyclical bias field having substantially a substantially spatially uniform zero average value; causing the magnetic moments to precess; receiving signals from the precessing magnetic moments; demodulating the received signals using demodulation signals; and processing the demodulated received signals to produce an image of the magnetic spins in the object.

Claim 3

The method as described in claim 1 where the step of polarizing the magnetic moments includes the step of applying a pulsed magnetic field to the object.

Claim 4

The method as described in claim 2 where the step of applying the gradient fields and the bias field to the object includes the step of applying the gradient fields and bias field in spatial quadrature to the pulsed magnetic field.

Claim 5

The method as described in claim 1 where the step of demodulating the received signals includes the step of deriving the frequency of the demodulation signals from the frequency of the cyclical bias field.

Claim 6

Apparatus for imaging the magnetic spin density in an object comprising: means for polarizing the magnetic moments in the object; means for applying gradient fields and a cyclical bias field having substantially a zero average value during the time signals are received; means for causing the magnetic moments to precess; means for receiving signals from the precessing magnetic moments; means for demodulating the received signals using demodulation signals; and means for processing the demodulated received signals to produce an image of the magnetic spins in the object.

Claim 7

Apparatus for imaging the magnetic spin density in an object comprising: means for polarizing the magnetic moments in the object; means for applying gradient fields and a cyclical bias field having substantially a zero average value during the time signals are received; means for causing the magnetic moments to precess; means for receiving signals from the precessing magnetic moments; means for demodulating the received signals using demodulation signals; and means for processing the demodulated received signals to produce an image of the magnetic spins in the object.

Claim 8

Apparatus as described in claim 5 where the cyclical bias field is a pulsed field having a trace period during which the received signals are acquired and a retrace period, of opposite polarity and substantially shorter duration.

Claim 9

Apparatus as described in claim 6 where the frequency of the pulsed bias field is substantially equal to the gyromagnetic constant multiplied by the value of the bias field during the trace period.

Claim 10

Apparatus as described in claim 6 where the frequency of the pulsed bias field is substantially equal to a submultiple of the gyromagnetic constant multiplied by the value of the bias field during the trace period.

Claim 11

Apparatus as described in claim 5 where the cyclical bias field is a symmetrical waveform spending substantially equal time periods in each polarity.

Claim 12

Apparatus as described in claim 9 where the cyclical bias field is substantially a sine wave.

Claim 13

Apparatus as described in claim 9 where the cyclical bias field is substantially a square wave.

Claim 14

Apparatus as described in claim 9 where the processing means includes polarity switching means for obtaining opposite polarities of the received signal during each half of the square wave and means for demodulating the polarity switched signal and the received signal using demodulating signals in quadrature phase.

Claim 15

Apparatus as described in claim 5 where the frequency of the demodulating signals are substantially equal to the frequency of the cyclical bias field.

Claim 16

Apparatus as described in claim 5 where the frequency of the demodulating signals are substantially equal to a multiple of the frequency of the cyclical bias field.

Claim 17

Apparatus as described in claim 5 including means for applying a static bias field for substantially a quarter of the period of time corresponding to the period represented by the difference of the gyromagnetic ratios of water and fat multiplied by the static bias field and where the processing means includes means for separating the demodulated received signals corresponding to water and fat.

Claim 18

Apparatus as described in claim 5 where the polarizing means, gradient fields and the cyclical bias fields all point in a first direction, and including a pulsed rf field pointing normal to the first direction which follows the polarizing means to initiate precession.

Claim 19

In a method for deriving spin-density information from precessing magnetic moments in an object with substantial immunity to inhomogeniety the steps of: applying a cyclically-varying bias field having substantially zero average value normal to the axis of the precessing moments; receiving signals from the precessing moments in the presence of the cyclical bias field; and demodulating the received signals using a demodulation signal based on the cyclically-varying bias field.

Claim 20

In a method for deriving spin-density information from precessing magnetic moments in an object with substantial immunity to inhomogeniety the steps of: applying a cyclically-varying bias field having substantially zero average value normal to the axis of the precessing moments; receiving signals from the precessing moments in the presence of the cyclical bias field; and demodulating the received signals using a demodulation signal based on the cyclically-varying bias field.