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Statistical Parametric Mapping
for fMRI, PET and VBM
Ged Ridgway
Wellcome Trust Centre for Neuroimaging
UCL Institute of Neurology
SPM Course
October 2011
Contents
 Historical background
 Positron emission tomography (PET)
 Statistical parametric mapping (SPM)
 Functional magnetic resonance imaging (fMRI)
 Voxel-based morphometry
Part I: 19th Century (!)
Angelo Mosso, Turin
1846 – 1910
Figures from
David Heeger
Part I: 19th Century (!)
 Early evidence for functional
segregation from damage
 E.g. Phineas Gage, 1823-
1860, studied by John Martyn
Harlow, 1819-1907.
“Previous to his injury he possessed a
well-balanced mind … the equilibrium
between his intellectual faculties and
animal propensities, seems to have
been destroyed. He is fitful, irreverent,
indulging in the grossest profanity”
From the collection of Jack and Beverly Wilgus
Haemodynamics
 Roy & Sherrington (1890), On the Regulation of the
Blood-supply of the Brain, J Physiol 11(1-2)
 Fulton (1928) Observations upon the vascularity of the
human occipital lobe during visual activity, Brain 51(3)
 Raichle (1998), PNAS 95(3):765-772
– “introduction of an in vivo tissue autoradiographic measurement
of regional blood flow in laboratory animals by Kety’s group
provided the first glimpse of quantitative changes in blood flow in
the brain related directly to brain function”
– William Landau [in Kety’s group]: “this is a very secondhand way
of determining physiological activity; it is rather like trying to
measure what a factory does by measuring the intake of water
and the output of sewage. This is only a problem of plumbing”
Haemodynamics
 Please see Kerstin
Preuschoff’s Zurich SPM
Course slides for more
Friston et al. (2000) NeuroImage 12:466-477
Positron emission tomography (PET)
 A tracer (radionuclide) emits a
positron, which annihilates with an
electron, emitting a pair of gamma
rays in opposite directions
 The detected lines can be
grouped into projection images
(sinograms) and reconstructed
into tomographic images
 Different tracers allow various
properties to be measured
– 15O can measure blood flow
relatively quickly (<1 min) but
requires a cyclotron because of its
short 2 minute half-life
– 18F Fluorodeoxyglucose (FDG)
measures glucose metabolism, and
has a half life of 110 minutes
– Other tracers exist that bind to
interesting receptors (e.g. dopamine,
serotonin) or beta-amyloid plaques
Parametric mapping
 Early PET focussed on
quantitation of parameters
 See also Lammertsma &
Hume (1996) [source of figure]
 Prof Terry Jones interviewed
by UCL Centre for History of
Medicine:
“It was as if I could take a bit of
my brain out and then put it
into a laboratory well counter
… how many megabecques or
microcuries of radioactivity per
ml of tissue … I pointed out if
we could measure the
concentration in the artery and
the tissue at the same time,
you could solve these
equations for blood flow and
oxygen consumption”
Statistical
parametric mapping
Often the interest is not
the quantities, but their
differences in different
conditions
Terry Jones: “And here
was this guy Friston,
sort of running
roughshod over all this
[quantitation], and
saying, ‘Oh, I’ll take five
of those, and five of
those, and look for
statistical differences…”
Statistical parametric mapping
Statistical parametric mapping
 Some questions you might ask at this point
– Can we test more interesting hypotheses than condition A vs. B?
• Answer: The general linear model and experimental design
– How significant is a particular voxel’s t-score, given
consideration of so many voxels over the brain?
• Multiple comparison correction using random field theory
– What if the subject moves during the scan or between scans?
How can we report locations of findings? How can we combine
data from multiple subjects?
• Image registration and spatial normalisation; hierarchical models
– What about functional integration of multiple brain regions?
• Functional and effective connectivity, dynamic causal modelling
Normalisation
Statistical Parametric Map
Image time-series
Parameter estimates
General Linear Model
Realignment Smoothing
Design matrix
Anatomical
reference
Spatial filter
Statistical
Inference
RFT
p <0.05
Functional magnetic resonance imaging (fMRI)
 Some disadvantages of PET
– Slow, even compared to haemodynamic delays
– Low spatial resolution
– Ionising radiation
 Magnetic resonance imaging
– Quantum mechanical property of spin, e.g. of hydrogen nuclei
– Spins align with and precess around an applied magnetic field
– Inputting RF energy perturbs the established equilibrium and
puts spins in phase with each other; a signal can be measured
– Spins relax back to equilibrium and de-phase with each other
• Different longitudinal (T1) and transverse (T2) relaxation times
• Field inhomogeneities accelerate the T2 relaxation (T2*)
Functional magnetic resonance imaging (fMRI)
 Blood contains oxygenated and deoxygenated
haemoglobin, with different magnetic properties
 Paramagnetic deoxyhaemoglobin distorts the magnetic
field, leading to faster T2* decay
 The influx of blood following activity changes the
proportion of oxy- and deoxyhaemoglobin, and hence
the T2 or T2*-weighted MRI signal
 This Blood Oxygenation Level Dependent (BOLD) effect
allows functional imaging with MRI
See also Kerstin’s slides and Ogawa & Sung (2007)
More on the BOLD effect
More Karl on the BOLD effect
 Friston (2009)
– How many times have you read, “We know very little about the
relationship between fMRI signals and their underlying neuronal
causes”?
– In fact, decades of careful studies have clarified an enormous
amount about the mapping between neuronal activity and
hemodynamics
– Furthermore, we know more than is sufficient to use fMRI for
brain mapping. This is because the statistical models used to
infer regionally specific responses make no assumptions about
how neuronal responses are converted into measured signals
The imaging bit of MRI…
 … is complicated!
 The rate of precesssion is field-strength dependent
 Electromagnetic coils can setup spatial gradients in field-
strength, which cause gradients in precession frequency
 A frequency gradient persisting for a certain time
establishes a sinusoidal phase gradient
 The overall signal is stronger if the spatial frequency of
the object (e.g. some cortical folds) matches this
 Can effectively measure the 2D Fourier transform or
spectrum of an object, and hence reconstruct an image
The imaging bit of MRI…
MRI from picture to
proton has one of the
clearest explanations
and some great
examples of how
spatial frequency
space (k-space)
relates to features in
the image space
Temporal modelling of fMRI data
 With PET we can acquiring some scans in one condition
and some in another, and test statistically for differences
 With fMRI, we typically acquire a scan every few
seconds, and wish to study “event-related” responses
– (also recently sub-second sampling, e.g. Feinberg et al., 2009)
 We do this by creating a model of what the
haemodynamic response to a sequence of events or
conditions would look like in time (with its ~6s delay,
undershoot, etc.) and fitting this model to the data
BOLD signal
Time
single voxel
time series
Voxel-wise time series analysis
Model
specification
Parameter
estimation
Hypothesis
Statistic
SPM
Multiple subjects and standard space
The Talairach Atlas
(single subject, post-mortem)
The MNI/ICBM AVG152 Template
(average of 152 in-vivo MRI)
Spatial normalisation
Computational anatomy
If we can estimate the
transformations that align and
warp each subject to match a
template, then we can study
individual differences in these
transformations or derivatives
E.g. deformation-based and
tensor-based morphometry
– Changes in local volume are
interesting and interpretable
Voxel based morphometry (VBM)
 VBM involves creating spatially normalised images,
whose intensities at each point relate to the local volume
of a particular brain tissue (e.g. gray matter) at the
corresponding point in the original (unnormalised) image
 This requires tissue segmentation, spatial normalisation,
and a “change of variables” to account for volume
changes occuring in the normalisation process
 Spatial smoothing helps to ameliorate residual
anatomical differences after imperfect normalisation
 The same general linear modelling & RFT machinery in
SPM can then be used to study differences in structure
Normalisation
Statistical Parametric Map
Image time-series
Parameter estimates
General Linear Model
Realignment Smoothing
Design matrix
Anatomical
reference
Spatial filter
Statistical
Inference
RFT
p <0.05
SPM Documentation
Peer reviewed literature
SPM Books:
Human Brain Function I & II
Statistical Parametric Mapping
Online help
& function
descriptions
SPM Manual

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01_Overview.pptx

  • 1. Statistical Parametric Mapping for fMRI, PET and VBM Ged Ridgway Wellcome Trust Centre for Neuroimaging UCL Institute of Neurology SPM Course October 2011
  • 2. Contents  Historical background  Positron emission tomography (PET)  Statistical parametric mapping (SPM)  Functional magnetic resonance imaging (fMRI)  Voxel-based morphometry
  • 3. Part I: 19th Century (!) Angelo Mosso, Turin 1846 – 1910 Figures from David Heeger
  • 4. Part I: 19th Century (!)  Early evidence for functional segregation from damage  E.g. Phineas Gage, 1823- 1860, studied by John Martyn Harlow, 1819-1907. “Previous to his injury he possessed a well-balanced mind … the equilibrium between his intellectual faculties and animal propensities, seems to have been destroyed. He is fitful, irreverent, indulging in the grossest profanity” From the collection of Jack and Beverly Wilgus
  • 5. Haemodynamics  Roy & Sherrington (1890), On the Regulation of the Blood-supply of the Brain, J Physiol 11(1-2)  Fulton (1928) Observations upon the vascularity of the human occipital lobe during visual activity, Brain 51(3)  Raichle (1998), PNAS 95(3):765-772 – “introduction of an in vivo tissue autoradiographic measurement of regional blood flow in laboratory animals by Kety’s group provided the first glimpse of quantitative changes in blood flow in the brain related directly to brain function” – William Landau [in Kety’s group]: “this is a very secondhand way of determining physiological activity; it is rather like trying to measure what a factory does by measuring the intake of water and the output of sewage. This is only a problem of plumbing”
  • 6. Haemodynamics  Please see Kerstin Preuschoff’s Zurich SPM Course slides for more Friston et al. (2000) NeuroImage 12:466-477
  • 7. Positron emission tomography (PET)  A tracer (radionuclide) emits a positron, which annihilates with an electron, emitting a pair of gamma rays in opposite directions  The detected lines can be grouped into projection images (sinograms) and reconstructed into tomographic images  Different tracers allow various properties to be measured – 15O can measure blood flow relatively quickly (<1 min) but requires a cyclotron because of its short 2 minute half-life – 18F Fluorodeoxyglucose (FDG) measures glucose metabolism, and has a half life of 110 minutes – Other tracers exist that bind to interesting receptors (e.g. dopamine, serotonin) or beta-amyloid plaques
  • 8. Parametric mapping  Early PET focussed on quantitation of parameters  See also Lammertsma & Hume (1996) [source of figure]  Prof Terry Jones interviewed by UCL Centre for History of Medicine: “It was as if I could take a bit of my brain out and then put it into a laboratory well counter … how many megabecques or microcuries of radioactivity per ml of tissue … I pointed out if we could measure the concentration in the artery and the tissue at the same time, you could solve these equations for blood flow and oxygen consumption”
  • 9. Statistical parametric mapping Often the interest is not the quantities, but their differences in different conditions Terry Jones: “And here was this guy Friston, sort of running roughshod over all this [quantitation], and saying, ‘Oh, I’ll take five of those, and five of those, and look for statistical differences…”
  • 11. Statistical parametric mapping  Some questions you might ask at this point – Can we test more interesting hypotheses than condition A vs. B? • Answer: The general linear model and experimental design – How significant is a particular voxel’s t-score, given consideration of so many voxels over the brain? • Multiple comparison correction using random field theory – What if the subject moves during the scan or between scans? How can we report locations of findings? How can we combine data from multiple subjects? • Image registration and spatial normalisation; hierarchical models – What about functional integration of multiple brain regions? • Functional and effective connectivity, dynamic causal modelling
  • 12. Normalisation Statistical Parametric Map Image time-series Parameter estimates General Linear Model Realignment Smoothing Design matrix Anatomical reference Spatial filter Statistical Inference RFT p <0.05
  • 13. Functional magnetic resonance imaging (fMRI)  Some disadvantages of PET – Slow, even compared to haemodynamic delays – Low spatial resolution – Ionising radiation  Magnetic resonance imaging – Quantum mechanical property of spin, e.g. of hydrogen nuclei – Spins align with and precess around an applied magnetic field – Inputting RF energy perturbs the established equilibrium and puts spins in phase with each other; a signal can be measured – Spins relax back to equilibrium and de-phase with each other • Different longitudinal (T1) and transverse (T2) relaxation times • Field inhomogeneities accelerate the T2 relaxation (T2*)
  • 14. Functional magnetic resonance imaging (fMRI)  Blood contains oxygenated and deoxygenated haemoglobin, with different magnetic properties  Paramagnetic deoxyhaemoglobin distorts the magnetic field, leading to faster T2* decay  The influx of blood following activity changes the proportion of oxy- and deoxyhaemoglobin, and hence the T2 or T2*-weighted MRI signal  This Blood Oxygenation Level Dependent (BOLD) effect allows functional imaging with MRI See also Kerstin’s slides and Ogawa & Sung (2007)
  • 15. More on the BOLD effect
  • 16. More Karl on the BOLD effect  Friston (2009) – How many times have you read, “We know very little about the relationship between fMRI signals and their underlying neuronal causes”? – In fact, decades of careful studies have clarified an enormous amount about the mapping between neuronal activity and hemodynamics – Furthermore, we know more than is sufficient to use fMRI for brain mapping. This is because the statistical models used to infer regionally specific responses make no assumptions about how neuronal responses are converted into measured signals
  • 17. The imaging bit of MRI…  … is complicated!  The rate of precesssion is field-strength dependent  Electromagnetic coils can setup spatial gradients in field- strength, which cause gradients in precession frequency  A frequency gradient persisting for a certain time establishes a sinusoidal phase gradient  The overall signal is stronger if the spatial frequency of the object (e.g. some cortical folds) matches this  Can effectively measure the 2D Fourier transform or spectrum of an object, and hence reconstruct an image
  • 18. The imaging bit of MRI… MRI from picture to proton has one of the clearest explanations and some great examples of how spatial frequency space (k-space) relates to features in the image space
  • 19. Temporal modelling of fMRI data  With PET we can acquiring some scans in one condition and some in another, and test statistically for differences  With fMRI, we typically acquire a scan every few seconds, and wish to study “event-related” responses – (also recently sub-second sampling, e.g. Feinberg et al., 2009)  We do this by creating a model of what the haemodynamic response to a sequence of events or conditions would look like in time (with its ~6s delay, undershoot, etc.) and fitting this model to the data
  • 20. BOLD signal Time single voxel time series Voxel-wise time series analysis Model specification Parameter estimation Hypothesis Statistic SPM
  • 21. Multiple subjects and standard space The Talairach Atlas (single subject, post-mortem) The MNI/ICBM AVG152 Template (average of 152 in-vivo MRI)
  • 23. Computational anatomy If we can estimate the transformations that align and warp each subject to match a template, then we can study individual differences in these transformations or derivatives E.g. deformation-based and tensor-based morphometry – Changes in local volume are interesting and interpretable
  • 24. Voxel based morphometry (VBM)  VBM involves creating spatially normalised images, whose intensities at each point relate to the local volume of a particular brain tissue (e.g. gray matter) at the corresponding point in the original (unnormalised) image  This requires tissue segmentation, spatial normalisation, and a “change of variables” to account for volume changes occuring in the normalisation process  Spatial smoothing helps to ameliorate residual anatomical differences after imperfect normalisation  The same general linear modelling & RFT machinery in SPM can then be used to study differences in structure
  • 25. Normalisation Statistical Parametric Map Image time-series Parameter estimates General Linear Model Realignment Smoothing Design matrix Anatomical reference Spatial filter Statistical Inference RFT p <0.05
  • 26. SPM Documentation Peer reviewed literature SPM Books: Human Brain Function I & II Statistical Parametric Mapping Online help & function descriptions SPM Manual