physics of mr image acquisition - dspace@mit …...physics of mr image acquisition hst-583, fall...
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Physics of MR Image AcquisitionHST-583, Fall 2002
• Review: - MRI: Overview - MRI: Spatial Encoding
• MRI Contrast: Basic sequences - Gradient Echo - Spin Echo - Inversion Recovery
HST.583: Functional Magnetic Resonance Imaging: Data Acquisition and Analysis Harvard-MIT Division of Health Sciences and Technology Dr. Jorge Jovicich
HST.583
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Overview of an MRI procedure
Tissue protons align
IMAGE
(equilibrium state)
RF pulses
Protons absorb
(excited state)
processes
Protons emit RF energy )
detection
Relaxation processes
Repeat
using magnetic field gradients
Subject
Safety screening
RAW DATA MATRIX Fourier transform
00 Bγω = Larmor EquationMagnetic field with magnetic field
RF energy
Relaxation
(return to equilibrium state
NMR signal
Spatial encoding
HST.583 S(t1,t2) S(x1,x2)
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Dynamics of the Magnetization
d r
M( t )
dt =
rM( t ) × γ
rBext ( t) −
( Mx i + My j) T2
* − (Mz − M0 )
T1
k
B0
M0
timeEquilibrium
RF
Equilibrium
signal 00 Bγω =
B0 B0 B0 B0
M0
M(t)M(t) M(t)
• Mathematical Description: precession + relaxation (Bloch equations)
NMR
• Geometrical description: damped precession
HST.583
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Spatial Encoding in MRI
Key concept: ω( r ) = γ (B0 + G.r)
• Slice Selection
• Frequency Encoding
• Phase Encoding
- Location - Thickness - Rephasing/Refocussing
- Fourier Transform - FOV - Gradient Echo Formation
- Phase / Frequency Equivalency - FOV
HST.583
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Slice Selection
• RF excitation (selective bandwidth) + magnetic field gradient
shape & duration bandwidth (bw)• RF pulse properties
frequency (wo)
∆z
z)
z
B Bo bw
w
zo
wo
Gz
ω( r ) = γ B0 + G.r( ) RF
Gz
Phase
• Magnetic field gradient (G • Schematically
Slice thickness (∆z): bw = γ Gz ∆z • Slice parameters Slice center (zo): wo = γ Gz zo
HST.583
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‘Pulse sequence’ so far
RF
“slice select” Gz
MR signalfrom whole S(t)
Selected slice
Sample points
t
t
T2 *
t
HST.583 Courtesy of L. Wald
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Frequency Encoding
• After slice selection all spins in the selected plane have the same frequency and phase (a)
• Signal is acquired while a magnetic field gradient Gx is on (b)
Gx
(a) (b) Gradient field y
63 MHz 64 MHz 65 MHz x
x
w(x) = γ Gx x
HST.583
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‘Pulse sequence’ so far
RF
“slice select” Gz
“freq. encode” Gx(read-out)
S(t)
Sample points t
t
t
t Signal dephases rapidly
HST.583 Courtesy of L. Wald
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More signal can be obtained:
RF
“slice select” Gz
“freq. encode” Gx(read-out)
S(t)
Sample pointst
-+
Acquisition window
Dephase
Rephase
We can save some time …HST.583
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‘Pulse sequence’ so far
RF
“slice select” Gz
“freq. encode” Gx(read-out)
S(t)
Sample points
HST.583
t
-
+
Acquisition window
Gradient Echo
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Frequency Encoding
Measured signal: Frequency spectrum: time domain 1D x-projection
S(t) Fourier transform
S(ω)
time
bw frequencyrec
δt Receiver bandwidth (bw )rec
Sampling time δt=1/ bwrec Nx: number of samples ω( r ) = γ (B0 + G.r)
Acquisition time (tacq): t = N δt = N / bwacq x x rec
• Relevant parameters Resolution (δx): δx = FOV / Nx x
Field of view (FOVx): bw = γ G FOVrec x x
HST.583
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We could have measured ‘exactly’the same information differently:
RF
“slice select” Gz
“freq. encode” Gx(read-out)
S(t)
Sample points t
-
+
Acquisition window
RF excitation sampling points
Each
So far we’ve used ONE and we’ve acquired Nx
while the read-out gradient was ON
HST.583
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Let’s look at one arbitrarysampled point in the MR signal
RF
Gz
Gx
S(t)
HST.583 dephasing during t Same net dephasing
-
+
t -
+ = -
-
RF
S(t)
Gz
Gx =
S(t) depends on net
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We can do the same for all Nx sampled points:
-
RF
Gz
Gx RF
Gz
Gx
+
RF
Gz
Gx
Measure one point after dephasing gradient
Net negative dephasing
Net zero dephasingRepeat experiment Nx
times to sample all points Net positive dephasingHST.583
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We could have measured ‘exactly’the same information differently:
S(t)
Measured signal: time domain
RF S(t)
slice Gzselect time
phase Gx FT
encode Frequency spectrum:
1D x-projection S(ω)
Repeat Nx times frequency
HST.583
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Basic Gradient Echo Sequence
RF α α
TR TE
Gz Slice
Gy Phase
Gx Read
HST.583
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Conventional spin-warpMRI sequence
θ Repeat Nphase times kphase
RF
GN
GNphase
slice
phase
phase
TE kreadGread
Signal Prephase
timet
0 acq
NNread TR Prephase
read
The signal we measure is in tγspatial frequency space (k-space) k(t ) = G(t ') dt '
2π ∫ 0 HST.583
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Pulse Sequences & Image Contrast
Contents: • Definition of Contrast • Contrast parameters • Concept of MRI contrast weighting • Properties of pulse sequences &
sequence parameters
HST.583
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Image Contrast Definition
• Goal: maximise the contrast ( USEFUL IMAGES! )
• Contrast: difference in MR signals between different tissues
Tissue 1 Tissue 2
Water protons’ T1, T2, T2*, ρ, T1, T2, T2*, ρ,mobility/environment: Diffusion, Flow Diffusion, Flow
MR signal: S1
noise
SSCNR σ
21 − =
S2
Some examples?Contrast to Noise ratio: HST.583
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Image Contrast: What can we manipulate?
Tissue Properties: fixed Experimental Variables
Tissue T1 (ms) T2 (ms) ρ* Fat 260 84 0.90 White Matter 780 90 0.72 Gray Matter 920 100 0.84 CSF 3000 300 1.00
• Pulse sequence
• Pulse sequence parameters
- Repetition time: TR
- Echo time: TE
ρ*: % H2O relative to CSF - Inversion time: TI
- RF flip angle: α
• Contrast agent
What’s the effect of these variables?
HST.583
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Image Contrast:Weighting the MR Signal
• General MRI pulse sequence: combination of contrasts
Signal Intensity: S(x,y) = k T1× ρ ×
× T2 × …
• Contrast Weighting: maximize one term, minimize the others
Example: T1-weighting T1
S(x,y) = k ρ× ×
× T2 × …
by choosing adequate sequence & sequence parameters
Some examples?HST.583
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Typical MRI sequences
Gradient Echo:- Proton Density weighting - T1 weighting - T2* weighting
Spin Echo:- Proton Density weighting - T1 weighting - T2 weighting - Double echo: PD & T2 weighting
Inversion Recovery:- MP-RAGE: for high T1 contrast - FLAIR: for PD or T2 weighting without CSF signal
HST.583
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Typical MRI sequences
Gradient Echo:- Proton Density weighting - T1 weighting - T2* weighting
Spin Echo:- Proton Density weighting - T1 weighting - T2 weighting - Double echo: PD & T2 weighting
Inversion Recovery:- MP-RAGE: for high T1 contrast - FLAIR: for PD or T2 weighting without CSF signal
HST.583
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Basic Gradient Echo Sequence
RF
Slice
Phase
Read
α α
TR TE
−
−−= *
21 0 expexp1sin
T TE
T TRMSGRE αMR Signal:
HST.583
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Repetition Time (TR): T1 contrast
TR encodeRF
Voltage(Signal)
Mxy
Mz
WM
GM
encode encode
GM: gray matter (long T1) time WM: white matter (short T1)
HST.583 Courtesy of L. Wald
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Gradient Echo Sequence
−
−−= *
21 0 expexp1sin
T TE
T TRMSGRE α
*
*
Proton Density weighting T1 weighting T2* weighting ( TR >>T1, short TE, sin α ~ 1 ) ( TR ~ T1, short TE, sin α ~ 1 ) ( TR >>T1, TE ~ T2* )
Water density Gray / White matter / CSF Hemorrhage
HST.583
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HST.583
Gradient Echo Sequence
FA = 3o
FA = 5o
FA = 30o
FLASH
Courtesy of A. Dale and B. Fischl
Manipulating contrast with flip angle
Proton Density Weighting T1 Weighting
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Typical MRI sequences
Gradient Echo:- Proton Density weighting - T1 weighting - T2* weighting
Spin Echo:- Proton Density weighting - T1 weighting - T2 weighting - Double echo: PD & T2 weighting
Inversion Recovery: - MP-RAGE: for high T1 contrast - FLAIR: for PD or T2 weighting without CSF signal
HST.583
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Basic Spin-Echo Sequence
Excitation Pulse Refocusing Pulse
τ τ
180o
90o
RF
Slice
TE Phase
Read
Spin EchoHST.583
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Spin-Echo Sequence: The MR Signal
τ τ
TE
TR
S TR TE
SE = M0 1 − exp − exp − T1 T2
HST.583
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Spin Echo Sequence
−
−−=
21 0 expexp1sin
T TE
T TRMSGRE α
Proton Density weighting T1 weighting T2 weighting ( TR >>T1, short TE, sin α ~ 1 ) ( TR ~ T1, short TE, sin α ~ 1 ) ( TR >>T1, TE ~ T2 )
Water density Gray / White matter / CSF Hemorrhage
HST.583
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Double Spin Echo Sequence
τ τ τ τ
180o 180o
90o
RF
Slice
TE1 TE2Phase
Read
Echo 1 Echo 2 HST.583
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Typical MRI sequences
Gradient Echo:- Proton Density weighting - T1 weighting - T2* weighting
Spin Echo:- Proton Density weighting - T1 weighting - T2 weighting - Double echo: PD & T2 weighting
Inversion Recovery:- MP-RAGE: for high T1 contrast - FLAIR: for PD or T2 weighting without CSF signal
HST.583
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Inversion Recovery
Excitation Pulse Refocusing Pulse Inversion Pulse
τ τ TI
180o 180o
90o
RF
Slice
TE Phase
Read
Magnetization Preparation Spin Echo
HST.583
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Enhanced T1-weighting: Inversion Recovery
M0
-Mo
Spin Echo
TE
Mz(t)
90o
180o180o TI
CSF GM
180o Inversion: prepare magnetization prior to Spin Echo detection
2/1/1/ )21(Signal eee −−− +−∝ ρ T TE T TR T TI
HST.583
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Fluid Attenuation Inversion Recovery (FLAIR)
M0
-Mo
Mz(t)
180o
TI
Spin Echo
TE
90o
180o
CSF
GM
Signal null at: TI = ln(2)* T1
HST.583
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Physics of MR Image AcquisitionHST-583, Fall 2002
• Review: - MRI: Overview - MRI: Spatial Encoding
• MRI Contrast: Basic sequences - Gradient Echo - Spin Echo - Inversion Recovery
HST.583