Systems and methods for designing multidimensional selective adiabatic pulses

• US 10,422,841 B2
• Filed: 04/21/2017
• Issued: 09/24/2019
• Est. Priority Date: 04/21/2016
• Status: Active Grant

• Current Assignee: Regents of The University of Minnesota (University of Minnesota)
• Original Assignee: Regents of The University of Minnesota (University of Minnesota)
• Inventors: Garwood, Michael, Jang, Woo Ju Albert
• Primary Examiner(s): Vargas, Dixomara
• Application Number:
  US15/493,959
• Publication Number:
  US 20170307708A1
• Time in Patent Office: 886 Days
• CPC Class Codes: G01R 33/4616 using specific RF pulses or specific modulation schemes, e.g. stochastic excitation, adiabatic RF pulses, composite pulses, binomial pulses, Shinnar-le-Roux pulses, spectrally selective pulses not being used for spatial selection
• CPC Class Codes: G01R 33/4836 using an RF pulse being spatially selective in more than one spatial dimension, e.g. a 2D pencil-beam excitation pulse
• CPC Class Codes: G01R 33/5602 by filtering or weighting based on different relaxation times within the sample, e.g. T1 weighting using an inversion pulse
• CPC Class Codes: G01R 33/5659 caused by a distortion of the RF magnetic field, e.g. spatial inhomogeneities of the RF magnetic field G01R33/56509, G01R33/56518, G01R33/56536 take precedence

Abstract

Described here are systems and methods for designing and implementing spatially selective, multidimensional adiabatic radio frequency (“RF”) pulses for use in magnetic resonance imaging (“MRI”). Spatially selective inversion can be achieved adiabatically in both two-dimensional (“2D”) and three-dimensional (“3D”) regions-of-interest. The multidimensional adiabatic pulses are generally designed using sub-pulses that are adiabatically driven using a parent adiabatic pulse.

Claims

1. A method for designing a multidimensional adiabatic radio frequency (RF) pulse waveform for use in magnetic resonance imaging (MRI), the steps of the method comprising:

(a) providing to a computer system;

a two-dimensional sub-pulse waveform to a computer system;

a first gradient waveform defining a magnetic field gradient along a first axis;

a second gradient waveform defining a magnetic field gradient along a second axis that is orthogonal to the first axis;

a parent adiabatic pulse waveform;

(b) computing with the computer system;

a first rephasing magnetic field gradient waveform to apply along the first axis, wherein the first rephasing magnetic field gradient has an area computed to zero an area under the first gradient waveform;

a second rephasing magnetic field gradient waveform to apply along the second axis, wherein the second rephasing magnetic field gradient has an area computed to zero an area under the second gradient waveform;

(c) discretizing the parent adiabatic pulse waveform using the computer system to generate a plurality of pulse segments, wherein discretizing the parent adiabatic pulse waveform includes spacing apart each pulse segment by a duration of time;

(d) producing with the computer system;

a multidimensional adiabatic pulse waveform by multiplying each of the plurality of pulse segments by the provided sub-pulse waveform; and

a gradient waveform set to be played out during the three-dimensional adiabatic pulse waveform by positioning the first and second magnetic field gradient waveforms to be played out during each pulse segment, and positioning the first and second rephasing magnetic field gradients to be played out during each duration of time between successive pulse segments.

2. The method as recited in claim 1, wherein step (d) includes performing a complex multiplication, such that each sub-pulse waveform is amplitude modulated by an amplitude of the corresponding pulse segment and such that a phase of the sub-pulse waveform is added with a phase of the corresponding pulse segment.

3. The method as recited in claim 1, wherein step (c) includes oversampling the parent adiabatic pulse waveform while discretizing the parent adiabatic pulse waveform.

4. The method as recited in claim 1, wherein the parent adiabatic pulse waveform provided in step (a) is an adiabatic full passage waveform.

5. The method as recited in claim 1, wherein step (b) further includes computing with the computer system, a magnetic field gradient blip waveform to apply along a third axis that is orthogonal to the first axis and the second axis, and wherein the gradient waveform set produced in step (d) includes positioning the magnetic field gradient blip to be played out during each duration of time between successive pulse segments.

6. The method as recited in claim 1, further comprising providing the multidimensional adiabatic pulse waveform and the gradient waveform set to a magnetic resonance imaging (MRI) system and operating the MRI system to generate a multidimensional adiabatic pulse using the multidimensional adiabatic pulse waveform and the gradient waveform set.

7. The method as recited in claim 6, further comprising acquiring k-space data with the MRI system after generating the multidimensional adiabatic pulse, and reconstructing an image from the acquired k-space data.

8. A method for imaging a subject using a magnetic resonance imaging (MRI) system with a parallel transmit radio frequency (RF) coil array to operate a pulse sequence that includes a multichannel adiabatic radio frequency (RF) pulse, the steps of the method comprising:

(a) providing to the MRI system, a different multichannel adiabatic RF pulse waveform for each coil in the parallel transmit RF coil array, wherein each multichannel adiabatic RF pulse waveform comprises a plurality of sub-pulse waveforms designed based on a weighting by a transmit sensitivity profile for the respective coil in the transmit RF coil array, and are spaced apart in time by a duration of time and driven by a discretized parent adiabatic pulse waveform for which the multichannel adiabatic RF pulse waveform is provided;

(b) providing gradient waveforms to the MRI system, wherein the gradient waveforms define magnetic field gradients to be generated during each sub-pulse waveform of the multichannel adiabatic RF pulse waveform;

(c) providing rephasing gradient waveforms to the MRI system, wherein the rephasing gradient waveforms define magnetic field gradients to be generated during the duration of time in between successive sub-pulse waveforms;

(d) generating a multichannel adiabatic RF pulse with the parallel transmit RF coil array by operating each coil using the provided different multichannel adiabatic RF pulse waveform for that coil,

(e) generating magnetic field gradients with the MRI system contemporaneously with the multichannel adiabatic RF pulse using the provided gradient waveforms and the provided rephasing gradient waveforms;

(f) acquiring data from a subject by sampling magnetic resonance signals generated in response to the multichannel adiabatic RF pulse; and

(g) reconstructing an image of the subject from the acquired data.

9. The method as recited in claim 8, wherein magnetic field rephasing gradients are played out during each duration of time along only a first gradient axis and a second gradient axis that is orthogonal to the first gradient axis, such that the multichannel adiabatic pulse waveform defines a two-dimensional adiabatic pulse.

10. The method as recited in claim 8, wherein a first rephasing magnetic field gradient is played out during each duration of time along a first gradient axis, a second rephasing magnetic field gradient is played out during each duration of time along a second gradient axis that is orthogonal to the first gradient axis, and a magnetic field gradient blip is played out during each duration of time along a third gradient axis that is orthogonal to the first and second gradient axes, such that the multichannel adiabatic pulse waveform defines a three-dimensional adiabatic pulse.

11. The method as recited in claim 8, wherein the multichannel adiabatic RF pulse refocuses transverse magnetization produced by generating an RF excitation pulse with the MRI system.

12. The method as recited in claim 11, wherein:

step (d) comprises generating an additional multichannel adiabatic RF pulse with the parallel transmit RF coil array by operating each coil using the provided different multichannel adiabatic RF pulse waveform for that coil;

step (e) comprises generating additional magnetic field gradients with the MRI system contemporaneously with the additional multichannel adiabatic RF pulse using the provided gradient waveforms and the provided rephasing gradient waveforms before acquiring the data in step (f);

and wherein the additional multichannel adiabatic RF pulse also refocuses the transverse magnetization produced by generating the RF excitation pulse with the MRI system.