IP Library Granted Patent US 9,903,928
Granted Patent B2
US 9,903,928 · App. 14/174,368 · Granted Feb 27, 2018

Beam steering with resonance along a trajectory

Inventors: Angela Lynn Styczynski Snyder (Minneapolis, MN); Carl J. Snyder (Minneapolis, MN); Michael G. Garwood (Medina, MN); J. Thomas Vaughan, Jr. (Stillwater, MN)
Assignee: Regents of the University of Minnesota
G01R33/4816G01R33/4833G01R33/5659G01R33/56536G01R33/56563
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Quick Facts
Patent No.
US 9,903,928
App. No.
14/174,368
Granted
Feb 27, 2018
Kind
B2
Abstract

A method for generating a magnetic resonance image includes configuring a magnetic field to correspond to a trajectory within a region of interest. The method includes applying RF excitation to spatially control a region of magnetic resonance corresponding to the trajectory. The method includes modulating the magnetic field coincident with the spatially controlled region of magnetic resonance. The method includes acquiring data corresponding to the region of magnetic resonance and generating an image based on the data.

Claims (24)

1. A method for producing an image with a magnetic resonance imaging (MRI) system comprising:

acquiring data from a subject by controlling the MRI system to:

generate one or more magnetic field gradients to define a resonance region in which spin isochromats are resonant at a resonance frequency, and wherein the one or more magnetic field gradients cause the resonance region to move in space along a trajectory;

generate a radio frequency (RF) field that is resonant with the resonance frequency by generating and dynamically adjusting at least one parameter of a plurality of independently adjustable RF pulses to steer a focal region of the RF field along the trajectory to be coincident with the resonance region;

acquire data from spin isochromats in the resonance region in response to applying the focal region of the RF field to the resonance region; and

reconstructing an image of the subject from the acquired data.

2. The method as recited in claim 1 , wherein the at least one parameter is selected from the group consisting of gain, phase, frequency, space, and time.

3. The method as recited in claim 1 , wherein the RF field comprises a frequency-swept pulse.

4. The method as recited in claim 3 , wherein the MRI system also generates magnetic field gradients during the frequency-swept pulse.

5. The method as recited in claim 1 , wherein the RF field comprises a gapped RF excitation.

6. The method as recited in claim 1 , wherein applying the magnetic field gradients includes increasing magnetic field inhomogeneities at a location different from the resonance region.

7. The method as recited in claim 1 , wherein the trajectory is at least one of a spiral trajectory, a circular trajectory, or a point trajectory.

8. The method as recited in claim 7 , wherein the trajectory comprises a plurality of circular trajectories that includes at least one of a series of concentric circles or a series of rotated and offset circles.

9. A radio frequency (RF) assembly for use in magnetic resonance, comprising:

an RF coil array having a plurality of RF coil elements for generating an RF field, wherein each RF coil element is independent of another RF coil element, each RF coil element having an input port;

an RF transmitter having a plurality of transmit channels wherein each transmit channel is coupled to an input port of one of the plurality of RF coil elements in the RF coil array, each transmit channel having at least one dynamically adjustable parameter to steer a focal region of the RF field through space along a trajectory;

a processor coupled to a magnetic resonance imaging (MRI) system and to the RF transmitter, the processor being configured to:

control the MRI system generate one or more magnetic field gradients in order to define a resonance region in which spin isochromats are resonant at a resonance frequency, and wherein the one or more magnetic field gradients cause the resonance region to move in space along a trajectory

control the RF transmitter to dynamically adjust the at least one dynamically adjustable parameter for each one of the plurality of RF coil elements in order to steer a focal region of the RF field along the trajectory to be coincident with the resonance region.

10. The RF assembly as recited in claim 9 , wherein each RF coil element is electrically independent of each other RF coil element in the RF coil array.

11. The RF assembly as recited in claim 9 , wherein each RF coil element in the RF coil array is supplied by an electrically independent control line.

12. The RF assembly as recited in claim 9 , wherein at least one of the RF coil elements in the RF coil array is electrically decoupled from another one of the plurality of RF coil elements in the RF coil array.

13. The RF assembly as recited in claim 9 , wherein the at least one parameter is selected from the group consisting of gain, phase, frequency, space, and time.

14. The RF assembly as recited in claim 13 , wherein the processor is configured to coordinate at least two of gain, phase, frequency, space, and time in moving the resonance region.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 8, 2015
From: SNYDER, ANGELA STYCZYNSKI; SNYDER, CARL; GARWOOD, MICHAEL; VAUGHAN, J. THOMAS
To: REGENTS OF THE UNIVERSITY OF MINNESOTA
Reel/Frame 035592/0096 →
CONFIRMATORY LICENSE Recorded Apr 1, 2015
From: UNIVERSITY OF MINNESOTA
To: NATIONAL INSTITUTES OF HEALTH (NIH), U.S. DEPT. OF HEALTH AND HUMAN SERVICES (DHHS), U.S. GOVERNMENT
Reel/Frame 035357/0124 →
Continuity (2)
Provisional Application 61761470 · Feb 6, 2013
Related Publication 20140218028A1 · Aug 7, 2014