Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI...

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Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Transcript of Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI...

Page 1: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Introduction to MRI Acquisition

James MeakinFMRIB Physics Group

FSL Course, Bristol, September 2012

1

Page 2: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

What are we trying to achieve?

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Page 3: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

What are we trying to achieve?

• Informed decision making:

• Protocols need to be tailored to the problem (Motion? Effect size? Area of activation?)

• Learning some physics will make this less daunting

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Page 4: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

What are we trying to achieve?

• Informed decision making:

• Protocols need to be tailored to the problem (Motion? Effect size? Area of activation?)

• Learning some physics will make this less daunting

• A common language:

• Explain your needs to physicists/radiographers

• Understand their response

• There is a LOT of jargon, but you can master it!

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Page 5: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

MRI Physics

• Today:

• Basics of (nuclear) Magnetic Resonance

• Image Formation

• Functional MRI

• The BOLD effect

• Acquisition and artefacts

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Page 6: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Nuclear Spin

• Some elementary particles (eg Hydrogen) exhibit “spin”

• Appear to rotate about an axis

• Charge + spin = magnetic moment

spin

H1

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Page 7: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Nuclear Spin

• Some elementary particles (eg Hydrogen) exhibit “spin”

• Appear to rotate about an axis

• Charge + spin = magnetic moment

spinN

S

H1

4

Page 8: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Nuclear Spin

• Some elementary particles (eg Hydrogen) exhibit “spin”

• Appear to rotate about an axis

• Charge + spin = magnetic moment

spinN

S

H1

4

Page 9: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Magnetic Fields (B)

No Field

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Page 10: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Magnetic Fields (B)

• What happens when you place a bunch of nuclei with spin into a magnetic field?

No Field

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Page 11: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Magnetic Fields (B)

• What happens when you place a bunch of nuclei with spin into a magnetic field?

Main B Field

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Page 12: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Magnetic Fields (B)

• What happens when you place a bunch of nuclei with spin into a magnetic field?

• On average, they’ll tend to align with the field (a net magnetic moment)

Main B Field

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Page 13: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Precession

• A force (Gravity or B Field) tries to tilt the spinning object

• But because of spin, the axis precesses instead of tilting

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Page 14: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• Energy pulse tips magnetisation away from B0

• ...if energy rotates at resonant frequency: RF pulse!

B0

ω0 = γB0

Excitation

courtesy of William Overall

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Page 15: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• Energy pulse tips magnetisation away from B0

• ...if energy rotates at resonant frequency: RF pulse!

B0

ω0 = γB0

Excitation

courtesy of William Overall

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Page 16: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• Once excited, magnetisation precesses at resonance frequency

B0

Precession

courtesy of William Overall

ω0 = γB0

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Page 17: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• Once excited, magnetisation precesses at resonance frequency

B0

Precession

courtesy of William Overall

ω0 = γB0

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Page 18: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• Changing magnetic field induces current in wire

• Precessing magnetisation detected with coil

• Can only detect component in transverse (xy) plane

B0

Signal detection

courtesy of William Overall

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Page 19: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• Changing magnetic field induces current in wire

• Precessing magnetisation detected with coil

• Can only detect component in transverse (xy) plane

B0

Signal detection

courtesy of William Overall

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Page 20: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Magnetic Resonance

• Magnetic: external field (B0) magnetises sample

• Usually detect hydrogen protons in water

• Potentially any element with spin (1H, 19F, 31P...)

• Resonance: magnetization has characteristic frequency

• Also called the “Larmour” frequency

• Proportional to the strength of the magnetic field the spin is in

• For protons, resonance frequency is in RF range

ω0 = γB0

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Page 21: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• Magnetization “relaxes” back into alignment with B0

• Speed of relaxation has time constants: T1 and T2

B0

Relaxation

courtesy of William Overall

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Page 22: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• Magnetization “relaxes” back into alignment with B0

• Speed of relaxation has time constants: T1 and T2

B0

Relaxation

courtesy of William Overall

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Page 23: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Mxy

Signal decaysaccording to T2

in transverse plane

Relaxation: T1 and T2

RF pulse

Time

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Page 24: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Echo time (TE) & T2 contrast

Echo time (TE)

Sig

nal

White matter

Gray matter

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Page 25: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

MRI Physics

• Today:

• Basics of (nuclear) Magnetic Resonance

• Image Formation

• Functional MRI

• The BOLD effect

• Acquisition and artefacts

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Page 26: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Making an image

B0

Differentiate between signal from different locations

magnet

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Page 27: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• Add a spatially varying magnetic field gradient (G)

• Field varies linearly along one direction

• Gradient field adds to or subtracts from B0

Making an image

B0G

Differentiate between signal from different locations

magnet

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Page 28: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• Resonance frequency is proportional to total field

B0

Precession

courtesy of William Overall

ω0 = γ(B0+ΔB)

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Page 29: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Magnetic gradients

Higherfrequency

Lowerfrequency

Higher field

Lower field

B0

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Page 30: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• Protons at each position precess at different frequencies

• RF coil hears all of the protons at once

• Distinguish material at a given position by selectively listening to that frequency

Magnetic gradients

Higherfrequency

Lowerfrequency

Higher field

Lower field

B0

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Page 31: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Decoding Frequency: The Fourier Transform

• Expresses a function of time as a function of frequency

• Imagine an orchestra: you differentiate between different instruments based on their frequency

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Page 32: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

The Fourier TransformA

mpl

itude

Fouriertransform

Time / s

Fouriertransform A

mpl

itude

Frequency / Hz

Bass

Cellos (loudest)

Violins

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Page 33: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

ImageSpace

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Page 34: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

ImageSpace

FourierTransform

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Page 35: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

Brightness = How much of thisspatial frequency is in your image

ImageSpace K-Space

FourierTransform

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Page 36: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

Brightness = How much of thisspatial frequency is in your image

ImageSpace K-Space

FourierTransform

Low Spatial Frequencies

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Page 37: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

Brightness = How much of thisspatial frequency is in your image

ImageSpace K-Space

FourierTransform

Low Spatial Frequencies

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Page 38: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

Brightness = How much of thisspatial frequency is in your image

ImageSpace K-Space

FourierTransform

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Page 39: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

Brightness = How much of thisspatial frequency is in your image

ImageSpace K-Space

FourierTransform

High Spatial Frequencies

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Page 40: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

Brightness = How much of thisspatial frequency is in your image

ImageSpace K-Space

FourierTransform

High Spatial Frequencies

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Page 41: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

Brightness = How much of thisspatial frequency is in your image

ImageSpace K-Space

FourierTransform

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Page 42: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

Brightness = How much of thisspatial frequency is in your image

ImageSpace K-Space

FourierTransform

Delete some spatial frequencies in the

LR direction

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Page 43: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

Brightness = How much of thisspatial frequency is in your image

ImageSpace K-Space

FourierTransform

Delete some spatial frequencies in the

LR direction

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Page 44: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Spatial frequencies

Brightness = How much of thisspatial frequency is in your image

ImageSpace K-Space

FourierTransform

Delete some spatial frequencies in the

LR direction

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Page 45: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

ky=0

kx=0

2D “k-space” describes contribution of each spatial frequency

xx

x

(2,1)

(0,4)

(8,1)

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Page 46: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

What does this have to do with MRI?

• Remember, we detect all excited protons in the object at the same time

• They’re resonating at different frequencies due to the gradients

• We acquire the data in k-space!

• We then fill k-space & Fourier transform it to get the image

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Page 47: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

• ➀ Excite magnetization (transmit RF pulse)

• ➁ Wait for time TE (“echo time”)

• ➂ Acquire signal from transverse magnetization (Mxy)

• ➃ Wait until time TR (“repetition time”)

• ➄ Repeat from ➀

RF

Acq

➀ ➁ ➂ ➃ ➄

TE

TR

Simple MRI “pulse sequence”

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Page 48: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Linescan (2DFT) Acquisition

Acquire one line after each excitationUseful for structural images (minimal artefacts)

kx

ky

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Page 49: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Linescan (2DFT) Acquisition

Acquire one line after each excitationUseful for structural images (minimal artefacts)

kx

ky

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Page 50: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Echo-planar Imaging (EPI) Acquisition

Acquire all of k-space in a “single shot”Used for FMRI, diffusion imaging

kx

ky

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Page 51: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Echo-planar Imaging (EPI) Acquisition

Acquire all of k-space in a “single shot”Used for FMRI, diffusion imaging

kx

ky

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Page 52: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

SNR =

Signal

!noise

Signal-to-noise ratio (SNR)Signal-to-noise ratio: describes signal “robustness”All else being equal, we want to maximise SNR!!

low SNRhigh SNR

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Page 53: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Signal-to-noise ratio (SNR)

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Page 54: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Protocol choices affecting SNR...

• RF receive coil & field strength

• Timing: TE & TR

• Voxel volume

• Scan duration

• Anything affecting signal!!!

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Page 55: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Protocol choices affecting SNR...

• RF receive coil & field strength

• Timing: TE & TR

• Voxel volume

• Scan duration

• Anything affecting signal!!!

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Page 56: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

What affects noise? Acquisition time

scan time

σnoise

Longer acquisition ⇒ less noise ⇒ higher SNR

SNR improves with the square root of scan time

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Page 57: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

What affects noise? Acquisition time

scan time

σnoise

Longer acquisition ⇒ less noise ⇒ higher SNR

SNR improves with the square root of scan time

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Page 58: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Larger voxels have signal from more tissue!

• Signal proportional to voxel volume

? 8xSNR

–2x2x2mm has 8x higher SNR than 1x1x1mm!

What affects signal? Voxel volume

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Page 59: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

? 8xSNR

Averaging to achieve high resolution

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Page 60: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

? 8xSNR

Can we recover lost SNR by averaging?Yes! But it requires a 64-fold increase in scan

time!

Averaging to achieve high resolution

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Page 61: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Contrast-to-noise ratio (CNR)

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Page 62: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

MRI Physics

• Today:

• Basics of (nuclear) Magnetic Resonance

• Image Formation

• Functional MRI

• The BOLD effect

• Acquisition and artefacts

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Page 63: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

Deoxyhemoglobin is the source of FMRI signal

Oxyhemoglobin: diamagnetic (same as tissue)Deoxyhemoglobin: paramagnetic (magnetic)

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Page 64: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

The BOLD Effect [ Ogawa et al, 1990 ]

Blood Oxygenation Level Dependent (BOLD) effect

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Page 65: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

The BOLD Effect [ Ogawa et al, 1990 ]

Blood Oxygenation Level Dependent (BOLD) effect

imaging voxel

Creates a range of frequencies in imaging voxel

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Page 67: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

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Page 68: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

HbO2

HbO2

HbO2

HbO2 dHb

dHb

HbO2

HbO2

dHbHbO2

HbO2

dHbdHb

HbO2

dHb = deoxyhemoglobinHbO2 = oxyhemoglobin

capillary

neuron

Vascular Response to Activation

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Page 69: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

HbO2

HbO2

HbO2

HbO2 dHb

dHb

HbO2

HbO2

dHbHbO2

HbO2

dHbdHb

HbO2

dHb = deoxyhemoglobinHbO2 = oxyhemoglobin

capillary

neuron

Vascular Response to Activation

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Page 70: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

HbO2

HbO2

HbO2

HbO2

O2 metabolism

dHb

dHb

HbO2

HbO2

dHbHbO2

HbO2

dHbdHb

HbO2

dHb = deoxyhemoglobinHbO2 = oxyhemoglobin

capillary

neuron

dHb

Vascular Response to Activation

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Page 71: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

O2 metabolism

dHb

dHb

HbO2

HbO2

dHbHbO2

HbO2

dHbdHb

HbO2

dHb = deoxyhemoglobinHbO2 = oxyhemoglobin

capillary

neuron

dHb

dHb

dHb

dHb

dHb

Vascular Response to Activation

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Page 72: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

O2 metabolism

dHb

dHb

HbO2

HbO2

dHbHbO2

HbO2

dHbdHb

HbO2

blood flow

HbO2

HbO2

HbO2

HbO2

HbO2HbO2

HbO2 HbO2

HbO2

HbO2HbO2

HbO2

HbO2

HbO2

dHb = deoxyhemoglobinHbO2 = oxyhemoglobin

capillary

neuron

dHb

HbO2

dHb

dHb

dHb

dHb

Vascular Response to Activation

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Page 73: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

O2 metabolism

dHb

dHb

HbO2

HbO2

dHbHbO2

HbO2

dHbdHb

HbO2

blood flow

HbO2

HbO2

HbO2

HbO2

HbO2HbO2

HbO2 HbO2

HbO2

HbO2HbO2

HbO2

HbO2

HbO2

dHb = deoxyhemoglobinHbO2 = oxyhemoglobin

capillary

blood volume

HbO2

HbO2HbO2

neuron

dHb

HbO2

HbO2

dHb

dHb

dHb

dHb

Vascular Response to Activation

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Page 74: Introduction to MRI Acquisition - fsl.fmrib.ox.ac.ukapps/fsl_MR_physics...Introduction to MRI Acquisition James Meakin FMRIB Physics Group FSL Course, Bristol, September 2012 1

O2 metabolism

dHb

dHb

HbO2

HbO2

dHbHbO2

HbO2

dHbdHb

HbO2

blood flow

HbO2

HbO2

HbO2

HbO2

HbO2HbO2

HbO2 HbO2

HbO2

HbO2HbO2

HbO2

HbO2

HbO2

[dHb]

dHb = deoxyhemoglobinHbO2 = oxyhemoglobin

capillary

blood volume

HbO2

HbO2HbO2

neuron

dHb

HbO2

HbO2

dHb

dHb

dHb

dHb

Vascular Response to Activation

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20 40 60 80

0.2

0.4

0.6

0.8

1.0

active

Echo time (TE, ms)

BO

LD

sig

na

l

rest

Typically, 1–5% signal change

Signal increases during activation (less decay)Signal change for longer delay (TE)

[dHb]

[dHb]

O2 use

bloodflow [dHb]

bloodvolume

BOLD Contrast

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20 40 60 80

0.2

0.4

0.6

0.8

1.0

active

Echo time (TE, ms)

BO

LD

sig

na

l

rest

20 40 60 80

0.2

0.4

0.6

0.8

1.0

active

Echo time (TE, ms)

BO

LD

sig

na

l

rest

difference(contrast)

Typically, 1–5% signal change

Signal increases during activation (less decay)Signal change for longer delay (TE)

O2 use

bloodflow [dHb]

bloodvolume

BOLD Contrast

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20 40 60 80

0.2

0.4

0.6

0.8

1.0

active

Echo time (TE, ms)

BO

LD

sig

na

l

rest

20 40 60 80

0.2

0.4

0.6

0.8

1.0

active

Echo time (TE, ms)

BO

LD

sig

na

l

rest

difference(contrast)

20 40 60 80

0.2

0.4

0.6

0.8

1.0

active

Echo time (TE, ms)

BO

LD

sig

na

l

rest

difference(contrast)

optimalrange

Typically, 1–5% signal change

Signal increases during activation (less decay)Signal change for longer delay (TE)

O2 use

bloodflow [dHb]

bloodvolume

BOLD Contrast

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Image artefacts worse at higher field strength

3T is currently a good tradeoff of signal vs artefacts

SNR and BOLD increase with field strength

BOLD signal and field strength (B0)

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Sources of BOLD Signal

Neuronal activity Metabolism

Blood flow

Blood volume

[dHb] BOLDsignal

Indirect measure of activity (via metabolism!)Subject’s physiological state & pathology can change

neurovascular coupling, muddying interpretation

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Stimulustiming

on

offtime

Hemodynamic response function (HRF)

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• Vascular response to activity is delayed & blurred

Stimulustiming

on

offtime

Hemodynamic response function (HRF)

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• Vascular response to activity is delayed & blurred

Stimulustiming

BOLDresponse

on

offtime

Hemodynamic response function (HRF)

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• Vascular response to activity is delayed & blurred

• Described by “hemodynamic response function”

• Limits achievable temporal resolution

• Must be included in signal model

Stimulustiming

BOLDresponse

on

offtime

Hemodynamic response function (HRF)

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Typical stimulus lasts 1–30 sRapid imaging: one image every few secondsAnatomical images take minutes to acquire!Acquire “single-shot” images (e.g., EPI)

1 23 …image TR

What is required of the scanner?

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Parameter Value Relevant points

TE(echo time)

1.5T: 60 ms3.0T: 30-40 ms7.0T: 15-20 ms

Determines functional contrast, set ≈T2*

TR(repeat time)

1–4 s HRF blurring < 1s;Poor resolution > 6s

Matrix size / Resolution

64x64 / 2-3 mm

Limited by distortion, SNR, FOV

Scan duration 2-60 mins Lower limit: sensitivity Upper limit: compliance

* Typical, not fixed!!Typical* FMRI Parameters

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• Noise: signal fluctuations leading to less robust detection with respect to statistical measures

Purely random noise(example: “thermal”)

Structured noise(example: “physiological”)

time

Confounds: Noise

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Confounds: Artefacts

Dropout Distortion

Artefacts: systematic errors that interfere with interpretability of data/images

“Ghosting”

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Source of signal dropout

BOLD contrast is based on signal dephasingBOLD imaging requires long delay (TE) for contrast

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Dephasing also occurs near air-tissue boundaries Sensitivity to BOLD effect reduces near air-tissue

boundaries

Source of signal dropout

sinus

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Long TEShort TE

Dephasing near air-tissue boundaries (e.g., sinuses)BOLD contrast coupled to signal loss (“black holes”)

Air-tissue effect is often larger than BOLD effect surrounding vessels!

BOLD Signal Dropout

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We think frequency maps to spatial location...So errors in frequency cause spatial mis-localization!

Field map

field offset local warping

EPI

Image distortion

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Non-BOLD fMRI

• BOLD depends on CBF, CBV, CMRO2

• Consider looking at these variables separately for longitudinal studies:

• CBF - Arterial Spin Labeling (ASL)

• CBV - Vascular Space Occupancy (VASO)

• CMRO2 - Calibrated BOLD

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Final Thoughts

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Final Thoughts

• Learn how different experimental parameters affect SNR and image artefacts

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Final Thoughts

• Learn how different experimental parameters affect SNR and image artefacts

• Tradeoffs: you can’t get something for nothing, but you do have options

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Final Thoughts

• Learn how different experimental parameters affect SNR and image artefacts

• Tradeoffs: you can’t get something for nothing, but you do have options

• Get to know a physicist/radiographer: get help setting up study protocols, show them your artefacts

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Final Thoughts

• Learn how different experimental parameters affect SNR and image artefacts

• Tradeoffs: you can’t get something for nothing, but you do have options

• Get to know a physicist/radiographer: get help setting up study protocols, show them your artefacts

• Quality assurance: always look at your data, even if you are running a well-tested protocol

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Acknowledgements

• Karla Miller for slides

• Previous years lecture (and more) available at www.fmrib.ox.ac.uk/~karla

• PractiCal fMRI (UC Berkeley) www.practicalfmri.blogspot.co.uk

• Animations: Spinbench

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Thank you!

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