IP Library Granted Patent US 9,541,624
Granted Patent B2
US 9,541,624 · App. 14/037,619 · Granted Jan 10, 2017

Method and apparatus for magnetic resonance imaging

Inventor: Cai Xia Fu (Shenzhen, CN)
Assignee: Siemens Aktiengesellschaft
G01R33/56527G01R33/5607G01R33/5613G01R33/56509
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Quick Facts
Patent No.
US 9,541,624
App. No.
14/037,619
Granted
Jan 10, 2017
Kind
B2
Abstract

In a method and apparatus for magnetic resonance imaging, a flip angle and/or inversion time of a spectrum suppression pulse is calculated according to a steady state condition of a longitudinal magnetization component of a spectrum composition suppressed by the spectrum suppression pulse and a zero crossing point condition of the longitudinal magnetization component. Raw magnetic resonance image data are acquired by applying a magnetic resonance imaging sequence that includes the spectrum suppression pulse provided with the flip angle and/or the inversion time.

Claims (71)

1. A method for acquiring magnetic resonance data, comprising:

in a processor, automatically calculating a flip angle and/or inversion time of a spectrum suppression pulse according to a steady state condition of a longitudinal magnetization component of a spectrum composition suppressed by a spectrum suppression pulse, to be generated in a magnetic resonance imaging sequence, and a zero crossing point condition of the longitudinal magnetization component;

operating a magnetic resonance data acquisition unit to acquire magnetic resonance data by applying said magnetic resonance imaging sequence comprising the spectrum suppression pulse provided with the flip angle and/or the inversion time, to a subject in the data acquisition unit;

entering said magnetic resonance data into memory locations in an electronic memory organized as k-space, and making k-space filled with said magnetic resonance data available in electronic form as a data file from said memory in a format suitable for further processing;

emitting the spectrum suppression pulse in the magnetic resonance imaging sequence before one or more excitation pulses and using, as the zero crossing point condition of the longitudinal magnetization component, making the longitudinal magnetization component of the spectrum composition zero before an excitation pulse corresponding to a center line of k-space; and

the inversion time comprising a first inversion time and a second inversion time, and calculating the flip angle or the inversion time of the spectrum suppression pulse, using a general formula, and the flip angle or the inversion time of the spectrum suppression pulse, wherein said general formula is:

{ E+F·C ·( D N-1 −1)/( D− 1)+ F·A·D N-1 }/(1− F·B·D N-1 )={ C ·( D KSpaceCenterLine-1 −1)/( D− 1)+ A·D KSpaceCenterLine-1 }/(− B·D KSpaceCenterLine-1 ),

where,

A=1−E Tl1

B=cos(β)·E Tl1

C=1−E Trep

D=cos(α)·E Trep

E=1−E Tr

F=cos(α)·E Tr

E Tl1 =exp(−Tl 1 /T 1 )

E Trep =exp(−Trep/T 1 )

E Tr =exp(−Tr/T 1 )

Tl 1 =Tl 1 Min+TlFill

Tr=TrMin+TrFill

α is a flip angle of an excitation pulse,

β is a flip angle of a spectrum suppression pulse,

T 1 is a longitudinal relaxation time of a spectrum composition suppressed by a spectrum suppression pulse,

N is the number of excitation pulses between two spectrum suppression pulses,

KSpaceCenterLine is the index number of a the center line of k-space,

TI 1 Min is the minimum time interval between the center of a spectrum suppression pulse and the center of a first excitation pulse following the spectrum suppression pulse,

Trep is the time between continuous excitation pulses,

TrMin is the minimum time interval between the center of the last excitation pulse in a pulse train and the center of a spectrum suppression pulse in a next pulse string of the magnetic resonance imaging sequence,

TIFill is the first inversion time, and

TrFill is the second inversion time.

2. A method as claimed in claim 1 , further comprising setting the first inversion time TIFill and the second inversion time TrFill as 0, and calculating the flip angle β in the step of calculating the flip angle or the inversion time of the spectrum suppression pulse.

3. A method as claimed in claim 1 , further comprising:

setting the flip angle β as 180 degrees; and

calculating the flip angle or the inversion time of the spectrum suppression pulse by setting the second inversion time TrFill as 0, and calculating the first inversion time TIFill.

4. A method as claimed in claim 3 , wherein, when the calculated first inversion time TIFill is smaller than 0, calculating the flip angle or the inversion time of the spectrum suppression pulse further by:

setting the first inversion time TIFill as 0, and

calculating the second inversion time TrFill.

5. A method as claimed in claim 1 , comprising: setting the flip angle β as 180 degrees; and

the step of calculating the flip angle or the inversion time of the spectrum suppression pulse by setting the first inversion time TIFill as 0, and calculating the second inversion time TrFill.

6. A method as claimed in claim 5 , wherein, when the calculated second inversion time TrFill is smaller than 0, calculating the flip angle or the inversion time of the spectrum suppression pulse further by:

setting the second inversion time TrFill as 0, and

calculating the first inversion time TIFill.

7. A magnetic resonance apparatus comprising:

a magnetic resonance data acquisition unit;

a processor configured to automatically calculate a flip angle and/or inversion time of a spectrum suppression pulse according to a steady state condition of a longitudinal magnetization component of a spectrum composition suppressed by a spectrum suppression pulse, to be generated in a magnetic resonance imaging sequence, and a zero crossing point condition of the longitudinal magnetization component;

a control unit configured to operate the magnetic resonance data acquisition unit to acquire magnetic resonance data by applying said magnetic resonance imaging sequence comprising the spectrum suppression pulse provided with the flip angle and/or the inversion time, to a subject in the data acquisition unit;

said control unit being configured to enter said magnetic resonance data into memory locations in an electronic memory organized as k-space, and to make k-space filled with said magnetic resonance data available in electronic form as a data file from said memory in a format suitable for further processing;

said control unit being configured to operate said magnetic resonance data acquisition unit to emit the spectrum suppression pulse in the magnetic resonance imaging sequence before one or more excitation pulses and using, as the zero crossing point condition of the longitudinal magnetization component, making the longitudinal magnetization component of the spectrum composition zero before an excitation pulse corresponding to a center line of k-space; and

the inversion time comprising a first inversion time and a second inversion time, and wherein said control unit is configured to calculate the flip angle or the inversion time of the spectrum suppression pulse, using a general formula, and the flip angle or the inversion time of the spectrum suppression pulse, wherein said general formula is:

{ E+F·C ·( D N-1 −1) ( D− 1)+ F·A·D N-1 }/(1 −F·B·D N-1 )={C·( D KSpaceCenterLine-1 −1)/( D− 1)+ A·D KspaceCenterLine-1 }/(− B·D KSpaceCenterLine-1 ),

where,

A=1−E TI1

B=cos(β)·E TI1

C=1−E Trep

D=cos(α)·E Trep

E=1−E Tr

F=cos(α)·E Tr

E TI1 =exp(−TI 1 /T 1 )

E Trep =exp(−Trep/T 1 )

E Tr =exp(−Tr/T 1 )

TI 1 =TI 1 Min+TIFill

Tr=TrMin+TrFill

α is a flip angle of an excitation pulse,

β is a flip angle of a spectrum suppression pulse,

T 1 is a longitudinal relaxation time of a spectrum composition suppressed by a spectrum suppression pulse,

N is the number of excitation pulses between two spectrum suppression pulses,

KSpaceCenterLine is the index number of a the center line of k-space,

TI 1 Min is the minimum time interval between the center of a spectrum suppression pulse and the center of a first excitation pulse following the spectrum suppression pulse,

Trep is the time between continuous excitation pulses,

TrMin is the minimum time interval between the center of the last excitation pulse in a pulse train and the center of a spectrum suppression pulse in a next pulse string of the magnetic resonance imaging sequence,

TIFill is the first inversion time, and

TrFill is the second inversion time.

Assignments (5)
CORRECTIVE ASSIGNMENT TO CORRECT THE ASSIGNEE PREVIOUSLY RECORDED AT REEL: 066088 FRAME: 0256. ASSIGNOR(S) HEREBY CONFIRMS THE ASSIGNMENT. Recorded Jan 17, 2024
From: SIEMENS HEALTHCARE GMBH
To: SIEMENS HEALTHINEERS AG
Reel/Frame 071178/0246 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 20, 2023
From: SIEMENS HEALTHCARE GMBH
To: SIEMENS HEALTHINEERS AG
Reel/Frame 066088/0256 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 30, 2017
From: SIEMENS AKTIENGESELLSCHAFT
To: SIEMENS HEALTHCARE GMBH
Reel/Frame 042524/0682 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 18, 2013
From: FU, CAI XIA
To: SIEMENS SHENZHEN MAGNETIC RESONANCE LTD
Reel/Frame 031805/0196 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 18, 2013
From: SIEMENS SHENZHEN MAGNETIC RESONANCE LTD
To: SIEMENS AKTIENGESELLSCHAFT
Reel/Frame 031805/0319 →
Priority Claims (1)
CN 2012 1 0362793 · Sep 26, 2012 · national
Continuity (1)
Related Publication 20140084922A1 · Mar 27, 2014