mri is a fourier transform magnetic resonance imaging · •this is not a physics lecture … but,...

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Page 1 Magnetic Resonance Imaging 6.003 Elfar Adalsteinsson with materials from LL Wald, MGH Martinos Center MRI is a Fourier Transform This is not a physics lecture … but, we’ll make plausibility arguments for the signal source and signal encoding in MRI that lead to this Fourier interpretation. !(#) = & ',) * +, ,- ./01(2 3 4 '52 6 4)) 7+7, MRI = Magnetic Resonance Imaging formerly known as Nuclear Magnetic Resonance Imaging Derives from (nuclear) spin angular momentum and associated magnetic dipole moment, m Proper treatment of spins: Quantum Mechanics Here: Classical picture “charged, spinning sphere” gives rise to current loop that creates a magnetic dipole moment, m Hydrogen 1 H Abundance ~ 80 M … MRI in medicine is imaging of water Signal Source in MRI Spins in a strong magnetic field, B0

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Page 1: MRI is a Fourier Transform Magnetic Resonance Imaging · •This is not a physics lecture … but, we’ll make plausibility arguments for the signal source and signal encoding in

Page 1

Magnetic Resonance Imaging

6.003

Elfar Adalsteinssonwith materials from LL Wald, MGH Martinos Center

MRI is a Fourier Transform

• This is not a physics lecture … but, we’ll make plausibility arguments for the signal source and signal encoding in MRI that lead to this Fourier interpretation.

!(#) = &',)

* +, , -./01(23 4 '526 4 ))7+7,

MRI = Magnetic Resonance Imaging

formerly known as

Nuclear Magnetic Resonance ImagingDerives from

(nuclear) spin angular momentumand associated magnetic dipole moment, m

Proper treatment of spins: Quantum Mechanics

Here:Classical picture

“charged, spinning sphere”

gives rise to current loopthat creates a magnetic dipole moment, m

Hydrogen 1HOther nuclei, 23Na, 31P, …much lower concentrations

Abundance~ 80 M

… MRI in medicine is imaging

of water

Signal Source in MRI

Spins in a strong magnetic field, B0

Page 2: MRI is a Fourier Transform Magnetic Resonance Imaging · •This is not a physics lecture … but, we’ll make plausibility arguments for the signal source and signal encoding in

Page 2

No net alignment:!M =

!m∑ = 0

Spins in earth’s magnetic field Spins in a strong, external field B0

B0 ~0.2T

Net alignment of spins in the presence of B0

yields signal source in MRI:!M =

!m∑

B0 ~0.2T

Spins in a strong, external field B0

Spins after RF excitation, B1

Direction of precession

Direction of B0

Spinning nucleus

Precession of Magnetization

xy

z

!Mxy

Mxy: Precesses at ω = γ "#

$ = "#'

Page 3: MRI is a Fourier Transform Magnetic Resonance Imaging · •This is not a physics lecture … but, we’ll make plausibility arguments for the signal source and signal encoding in

Page 3

Signal Detection

Faraday detection: a generator

( ) ( )0 cost M twF µ

0

( )( )

( ) sin( )

d tV tdt

V t M tw w

F= -

µ -

V(t)

Imaging

Image Encoding

What is imaging?

We want to estimate Mxy as a function of x, y, z …

How do we do this?

Image encoding embeds spatial information in FIDs

Image reconstruction infers spatial mapping from encoded FIDs

Can we do imaging with precessing spins in a B0 field?

Gradient Fields for

Frequency Encoding of Spatial Information

We introduce intentional spatial variation in the precession frequency of spins

Frequency and spatial location map 1-to-1 in the presence of a constant gradient field

Thus, piano comparison to frequency encoding

X-gradient coil produces a linearly varying z-directed field that is characterized by its slope, !", as a function of x,

!B(x, y, z) = B0 z Gx ⋅ x   z

!B(x, y, z) = (B0 +Gx ⋅ x)z

Bz

x

Bz

x

Bz

x

Gx =∂Bz∂x

Uniform magnet Field from x-gradient coil

Total field, sumof#$ and !" % &directed along (

Page 4: MRI is a Fourier Transform Magnetic Resonance Imaging · •This is not a physics lecture … but, we’ll make plausibility arguments for the signal source and signal encoding in

Page 4

Uniform magnet Field from x-gradient coil

Gx =∂Bz∂x

Bz

x

Bz

x

Bz

x

X-gradient coil produces a linearly varying z-directed field that is characterized by its slope, !", as a function of x,

!B(x, y, z) = B0 z Gx ⋅ x   z

!B(x, y, z) = (B0 +Gx ⋅ x)z

Total field, sumof#$ and !" % &directed along (

Nobel Prize

MR Nobel prizes:1943 physics, Stern1944, physics, Rabi1952, physics, Bloch, Purcell1991, Chemistry, Ernst2002, Chemistry, Wurthrich2003, Medicine, Lauterbur, Mansfield

Precession: ! = #(%& +∆%), or * = +,-(%& +∆%)

A gradient field, ./, maps space to frequency

After demodulation

i.e. ! =!& +#∆%, or * = *& + +,-∆%

∆% from ./: ! = !& +#./1, or * = *& + +,-./1

! = #./1, or * = +,-./1

Precession: ! = #(%& +∆%), or * = +,-(%& +∆%)

A gradient field, ./, maps space to frequency

After demodulation

i.e. ! =!& +#∆%, or * = *& + +,-∆%

∆% from ./: ! = !& +#./1, or * = *& + +,-./1

! = #./1, or * = +,-./1

!"($) = '(,*

+ ,, - ./01((,*,2)3,3-

The MRI Signal Equation

What’s is the phase term,4(,, -, $)?

By definition of phase, and by Larmor relation:

5152 = 6 = 789 ,

!"($) = '(,*

+ ,, - ./01((,*,2)3,3-

The MRI Signal Equation

What’s is the phase term, 4(,, -, $)?

By definition of phase, and by Larmor relation:

51((,*,2)52 = 6(,, -, $) = 789(,, -, $),

Page 5: MRI is a Fourier Transform Magnetic Resonance Imaging · •This is not a physics lecture … but, we’ll make plausibility arguments for the signal source and signal encoding in

Page 5

!"($) = '(,*

+ ,, - ./01((,*,2)3,3-

The MRI Signal Equation

What’s is the phase term, 4(,, -, $)?

i.e.

4(,, -, $) = ∫627 ,, -, 8 38 = 9∫6

2:; ,, -, 8 38

!"($) = '(,*

+ ,, - ./01((,*,2)3,3-

The MRI Signal Equation

What’s is the phase term, 4(,, -, $)?

If 56 ,, -, $ = 57 +9( $ , +9* $ -, then

4 ,,-, $ = :57$ +:;

7

29( < ,3< +

:;7

29* < -3<

!(#) = &',)

* +, , -./01(23 4 '526 4 ))7+7,

The MRI Signal Equation

where

8' # = 901∫;

4<' = 7=

8) # = 901∫;

4<) = 7=

After demodulation,

!

"

#$

#%&(#$, #%)

Fourier0(!, ")

Lab: Given raw data in k-space,reconstruct an image