Method of designing pulse sequences for parallel-transmission magnetic resonance imaging, and a method of performing magnetic resonance imaging using such sequences

Patent metadata

Field	Value
Publication number	US-10459056-B2
Application number	US-201615754273-A
Country	US
Kind code	B2
Filing date	Sep 28, 2016
Priority date	Oct 6, 2015
Publication date	Oct 29, 2019
Grant date	Oct 29, 2019

Abstract

A method of designing a pulse sequence for parallel-transmission magnetic resonance imaging comprises: a) acquiring, for each member of a cohort, inhomogeneity maps of radio-frequency fields generated within the member; b) computing, for each member of the cohort, a spatial distribution of flip angles of nuclear spins obtained using the pulse sequences, and c) computing a single cost or merit function representative of a difference between the spatial distributions of flip angles and a target distribution, and iteratively adjusting design parameters of the pulse sequences to optimize the cost or merit function; the steps b) and c) being carried out iteratively using a computer. A method of performing parallel-transmission magnetic resonance imaging on a subject using a pulse sequence designed by such a method is provided.

First claim

The invention claimed is:

1. A method of designing a pulse sequence for parallel transmission magnetic resonance imaging, said pulse sequence comprising at least a magnetic field gradient waveform and a set of radio-frequency pulses, each pulse of said set and said or each said magnetic field gradient waveform being defined by a plurality of design parameters and being associated to a respective transmission channel (RFC1-RFC8) of a parallel-transmission magnetic resonance imaging apparatus, the method comprising:
a) acquiring, for each member of a cohort of magnetic resonance imaging subjects, and for each of said transmission channels of said parallel transmission magnetic resonance imaging apparatus, an inhomogeneity map of the radio-frequency field generated within said member by one said transmission channels;
b) computing, for each member of said cohort and by taking the corresponding inhomogeneity maps as inputs, a spatial distribution of flip angles of nuclear spins obtained by playing said radio-frequency pulses on the respective transmission channels (RFC1-RFC8) while applying said magnetic field gradient waveform; and
c) computing a single cost or merit function representative of a difference between at least a plurality of said spatial distributions of flip angles and a target distribution of flip angles, and adjusting the design parameters of said radio-frequency pulses and of said gradient waveform to optimize said cost or merit function; said steps b) and c) being carried out iteratively using a computer.

2. The method according to claim 1 wherein said cost or merit function is chosen among:
a normalized root mean square error of the nuclear spin flip angle, averaged on at least a plurality of members of said cohort, or its reciprocal;
a normalized maximum root mean square error of the nuclear spin flip angle across the members of said cohort, or its reciprocal; and
a monotone function thereof.

3. The method according to claim 1 , wherein said step c) comprises iteratively adjusting said design parameters to optimize said cost or merit function under power constraints.

4. The method according to claim 3 , wherein said power constraints include local SAR constraints.

5. The method according to claim 1 , wherein said step a) further comprises acquiring, for each member of said cohort of magnetic resonance imaging subjects, an inhomogeneity map of a stating magnetic field within said member; and said step b) comprises taking said inhomogeneity maps as additional inputs for computing said spatial or statistical distributions of flip angles of nuclear spins.

6. The method according to claim 1 , wherein the control parameters of said radio-frequency pulses include temporal samples of an amplitude and a phase of each pulse.

7. The method according to claim 1 , applied to magnetic resonance imaging of human heads in a static magnetic field having amplitude of at least 3 T, preferably of at least 5 T and even more preferably of at least 7 T.

8. The method according to claim 1 wherein said target distribution of flip angles includes, in a region of space, flip angles of at least 70°.

9. A method of building a database of pulse sequences for parallel-transmission magnetic resonance imaging, the method comprising:
providing a plurality of magnetic resonance imaging subjects;
grouping said subjects into a plurality of cohorts according to at least one morphological feature; and
for each of said cohorts, designing a respective pulse sequence and a respective gradient waveform by a method according to claim 1 .

10. The method of performing parallel-transmission magnetic resonance imaging of a subject, comprising:
providing a database (DB) of pulse sequences and gradient waveforms, built using a method according to claim 9 ;
associating the subject to a cohort used for building said database on the basis of at least one morphological feature, a pulse sequence corresponding to said cohort; and
performing parallel-transmission magnetic resonance imaging using said pulse sequence;
wherein the method does not comprise a step of acquiring inhomogeneity maps for the subject and using them for designing the pulse sequence and the gradient waveform.

11. A method of performing parallel-transmission magnetic resonance imaging of a subject using a pulse sequence and a gradient waveform designed by a method according to claim 1 , wherein the subject does not belong to the cohort considered for designing the pulse sequence and the gradient waveform, and wherein the method does not comprise a step of acquiring inhomogeneity maps for the subject and using them for designing the pulse sequence and the gradient waveform.

Assignees

• Commissariat Energie Atomique

Inventors

• Boulant Nicolas
• Gras Vincent

Classifications

• G01R33/4833

  using spatially selective excitation of the volume of interest, e.g. selecting non-orthogonal or inclined slices · CPC title

• G01R33/4822

  in three dimensions · CPC title

• G01R33/5612 Primary

  Parallel RF transmission, i.e. RF pulse transmission using a plurality of independent transmission channels · CPC title

• G01R33/5659

  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) · CPC title

• G01R33/246

  Spatial mapping of the RF magnetic field B1 · CPC title