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Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

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Page 1: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Functional MRI

Daniel Bulte

Centre for Functional Magnetic Resonance Imaging of the Brain

University of Oxford

Page 2: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Overview

BOLD Contrast Metabolic and cerebral blood flow response Mechanism of MR signal change

Neurovascular coupling

Noise

Factors affecting BOLD More detail Changing physiological baseline

Metabolic modelling

Page 3: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

“Activation”

Page 4: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Deoxy-Haemoglobin

paramagnetic

different to tissue=0.08ppm

Page 5: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Oxy-Haemoglobin

diamagnetic

same as tissue

Page 6: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Field homogeneity & oxygenation state

Red blood cell 6 m diameter, 1-2 m thick

Susceptibility An object with differing magnetic properties distorts the field

Page 7: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Water

Freely diffusing water is the source of image signal

Two water spaces Intravascular (blood)

Capillaries and venules Extravascular - a larger pool

In 50ms (FMRI TE) water diffuses 4 capillary diameters

Page 8: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Magnetic field in a vessel

B0

r

a

Inside Cylinder

' = 2(1-Y) '

∆cos2

Page 9: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Magnetic field around a vessel

B0

r

a

Inside Cylinder

' = 2(1-Y) '

Outside Cylinder

∆cos2

r,

sin2a/r2cos

Page 10: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Vessel orientation Field inside and outside depends on angle

with respect to B0

Bandettini and Wong. Int. J. Imaging Systems and Technology. 6:133 (1995)

Page 11: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Blood oxygenation Field inside and outside depends on Y,

oxygenation

Bandettini and Wong. Int. J. Imaging Systems and Technology. 6:133 (1995)

Page 12: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Signal dependence Macroscopic behaviour of NMR, gradient echo

signal

More extravascular at high field

BOLD signal depends on the amount of dHb in the voxel

R2* = 4.3 (1-Y) B0 CBV

R2* = 0.04 {(1-Y)}2 B02 CBV

(venules, larger vessels)

(smaller capillaries)

Page 13: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

BOLD signal

Blood Oxygen Level Dependent signal

T2* change from the haemodynamic perturbation associated with neural activation

Page 14: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Neural activity Signalling Vascular response

Vascular tone (reactivity)Autoregulation

Metabolic signalling

BOLD signal

glia

arteriole

venule

B0 field

Synaptic signalling

Blood flow,oxygenationand volume

From neural activity to BOLD signal

Page 15: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Factors affecting BOLD signal?

Physiology Cerebral blood flow (baseline and change) Metabolic oxygen consumption Cerebral blood volume

Equipment Static field strength Field homogeneity (e.g. shim dependent T2*)

Pulse sequence Gradient vs spin echo Echo time, repeat time, flip angle Resolution

Page 16: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Deoxy-haemoglobin

Deoxy-haemoglobin

Oxy-haemoglobin

Oxy-haemoglobin

NeuralActivity

OxygenConsumption ImageImage

T2* weighted signalT2* weighted signal

Deoxy-haemoglobin

Deoxy-haemoglobin

Oxy-haemoglobin

Oxy-haemoglobin

NeuralActivity

OxygenConsumption ImageImage

T2* weighted signalT2* weighted signal

Deoxy-haemoglobin

Deoxy-haemoglobin

Oxy-haemoglobin

Oxy-haemoglobin

NeuralActivity

OxygenConsumption ImageImage

T2* weighted signalT2* weighted signal

Deoxy-haemoglobin

Deoxy-haemoglobin

Oxy-haemoglobin

Oxy-haemoglobin

NeuralActivity

OxygenConsumption ImageImage

T2* weighted signalT2* weighted signal

Deoxy-haemoglobin

Deoxy-haemoglobin

Oxy-haemoglobin

Oxy-haemoglobin

NeuralActivity

OxygenConsumption ImageImage

BloodFlow

BloodVolume

T2* weighted signalT2* weighted signal

Deoxy-haemoglobin

Deoxy-haemoglobin

Oxy-haemoglobin

Oxy-haemoglobin

NeuralActivity

OxygenConsumption ImageImage

BloodFlow

BloodVolume

T2* weighted signalT2* weighted signal

Deoxy-haemoglobin

Deoxy-haemoglobin

Oxy-haemoglobin

Oxy-haemoglobin

NeuralActivity

OxygenConsumption ImageImage

BloodFlow

BloodVolume

T2* weighted signalT2* weighted signal

Deoxy-haemoglobin

Deoxy-haemoglobin

Oxy-haemoglobin

Oxy-haemoglobin

NeuralActivity

OxygenConsumption ImageImage

BloodFlow

BloodVolume

T2* weighted signalT2* weighted signal

Deoxy-haemoglobin

Deoxy-haemoglobin

Oxy-Oxy-haemoglobinhaemoglobin

NeuralActivity

OxygenConsumption ImageImage

BloodFlow

BloodVolume

T2* weighted signalT2* weighted signal

Deoxy-haemoglobin

Deoxy-haemoglobin

Oxy-haemoglobin

Oxy-haemoglobin

NeuralActivity

OxygenConsumption ImageImage

BloodFlow

BloodVolume

T2* weighted signalT2* weighted signal

Deoxy-haemoglobin

Deoxy-haemoglobin

Oxy-haemoglobin

Oxy-haemoglobin

NeuralActivity

OxygenConsumption ImageImage

BloodFlow

BloodVolume

T2* weighted signalT2* weighted signal

Page 17: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Haemodynamic changes underlying BOLD

time

BO

LD

res

pons

e, %

initialdip

positiveBOLD response

post stimulusundershootovershoot

1

2

3

0

stimulus

CBF

CBV

CMRO2

stimulus

Page 18: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

BOLD contrast

Transverse relaxation Described by a time constant Time for NMR signal to decay

Loss of spins phase coherence (out of step) Spin echo, T2

Time varying field seen by diffusing spins Gradient echo, T2*

Time varying field seen by diffusing spins … plus spatial field variation across voxel

Why is magnetic field non uniform?

Page 19: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Modelling of the BOLD effect

Effects of oxygenation on T2* Ogawa et al., J. Biophys., 64:803-812 (1993) Kennan et al., MRM, 31:9-21 (1994) Boxerman et al., MRM, 34:4-10 (1995)

Flow and oxygenation coupling Buxton and Frank, JCBFM, 17:64-72 (1997)

CBV effects Buxton et al., MRM, 39:855-864 (1998) Mandeville et al., JCBFM, 19:679-689 (1999)

Page 20: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Signal evolution Monte Carlo simulation

Signal dephasing in the vascular tree amongst vessels of differing size, oxygenation and orientation

Boxerman J. et al. MRM 1995

Deoxy-Hb contribution to relaxation

Gradient echo S = Smax . e-TE/R2*

R2* (1-Y) CBVY=O2 saturationb~1.5

Page 21: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Echo time and BOLD sensitivity

• BOLD contrast-to-noise optimised when TE~T2*• T2* shorter at higher field

TE (ms)

RelativeCNR

TE optimization similar to T2 structural optimizations, just between different states rather than different tissues

Page 22: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Vessel density

500 m

100 m

Harrison RV et al. Cerebral cortex. 2002

Page 23: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Arteriole

100 m

Page 24: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Even smaller

50 m

Page 25: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Arterial side

Capillaries are randomly orientated

Oxygen exchange in capillaries

Arterioles perform local CBF controlArtery

Blood oxygen saturation, 98-100%

Arterioles 25 m 15% of CBV

Capillaries8 m 40% CBV

Page 26: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Venous side Venules

are (approx) randomly orientated

have the same blood volume as capillaries

have twice the deoxyHb concentration of capillaries

are more (para)magnetic than capillaries and arteries

VeinBlood oxygen saturation (resting), 60%

Venules 25-50 m 40% of CBV

Capillaries

Page 27: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

ActivationRest

Active: 50% increase in CBF, 20% increase in CMRO2

O2 Sat 100% 80% 60%

O2 Sat 100% 86% 72%

Page 28: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Decrease in deoxy-Hb concentration

Page 29: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

BOLD FMRIBasal (resting) state

capillary bed

venulesarterioles

= HbO2

= Hbr

FLOW

CBV

Field gradients

capillary bed

venulesarterioles

= HbO2

= Hbr

MRI signal

electricalactivity

hemodynamicresponse

x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x

- normal flow- basal level [Hbr]- basal CBV- normal MRI signal

Page 30: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

BOLD FMRI

capillary bed

venulesarterioles

= HbO2

= Hbr

FLOW

CBV

Activated state

capillary bed

venulesarterioles

= HbO2

= Hbr

FLOW

CBV

MRI signal

electricalactivity

hemodynamicresponse

x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x

- increased flow- decreased [Hbr] - increased CBV- increased MRI signal

Page 31: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Dissecting BOLD

SBOLD=f(CBV,CBF,CMRO2)

Buxton et al. Neuroimage 2004

Purer measures of neuronal activity?

Page 32: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

FMRI Modelling: TheHaemodynamic Response

The stimulus is convolved with an assumed or modeled impulse response function, the haemodynamic response function (HRF), to give the assumed BOLD response

Page 33: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

HRF

Stimulus (Single Event)

Haemodynamic Response Function (HRF)

0 10 20 30 seconds

The haemodynamic response to a stimulus is blurred and delayed

Time

Page 34: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Predicted Response The process can be modeled by convolving the

activity curve with the HRF

HRF Predicted neural activity

Predicted response

=

Page 35: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

GLM

Standard GLM Analysis: Correlate model at each voxel separately Measure residual noise variance T-statistic = model fit / noise amplitude Threshold T-stats and display map

Signals of no interest (e.g. artifacts) can affect both activation strength and residual noise variance

Use pre-processing to reduce/eliminate some of these effects

Page 36: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

A typical scan at 3T…

Gradient echo EPI

TR 2000 – 4000 ms

TE 30 ms

Flip angle 60 – 90 degrees

64 x 64

4 – 8 mm thick slices

20 – 40 slices

Page 37: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Why EPI?

A typical T2-weighted imaging series requires that TR be two to three times longer than the intrinsic tissue magnetization parameter, T1.

The T1 of biological samples is typically on the order of a second; TR must therefore be 3 seconds or more.

A typical MR image is formed from 128 repeated samples, so that the imaging time for our canonical T2 weighted scan is about 384 seconds, or more than 6.5 minutes.

By comparison, the EPI approach collects all of the image data, for an image of the same resolution, in 40 to 150 milliseconds

A nearly 10,000-fold speed gain!

Page 38: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

However…

Bandwidth and Artifacts

Chemical Shift

Shape Distortion

Ghosting

Resolution

Page 39: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Purer physiological measures

Perfusion and perfusion change

CMRO2 change

Cerebral blood volume

Oxygen extraction fraction

Page 40: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

neuronal activity- excitatory- inhibitory- soma action potential

metabolic response- glucose consumption- oxygen consumption

hemodynamic response- blood flow- blood volume- blood oxygenation

autoradiography

FDG PET

NIRS

H215O PET

FMRI

optical imaging

electrophysiology

EEG

MEG

Neurovascular coupling

Correlates of brain activity

Page 41: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Oxidative metabolism attenuates BOLD signal

Hoge R et al

CBF BOLD

Page 42: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

CMRO2 measurement

R2*(BOLD) = k CBV [dHb]

• k = field dependent constant• CBV = cerebral blood volume fraction• [dHb] = concentration of dHb in blood = theoretical CBV dependence (=1) = theoretical [dHb] dependence

1.5 (1.5T) [Boxerman et al, 1995] 1 (>3T) [Ogawa et al, 1993]

Measured

BOLD

Page 43: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

[dHb] = CMRO2 / CBF

Substitutions:

(Fick’s principle)

CBV (Grubb et al., 1974)

= 0.38 (steady state value)

CBV0 CBF0

CBF =

CMRO2 = CBF. OEF . Ca

ASL measured

CMRO2 measurement

Page 44: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

R2*(BOLD)

R2*0(BOLD) CMRO2(0)

CMRO2

CBF0

CBF 1 - ]=

Calibrate R2*0 using a hypercapnia challenge

CMRO2 measurement

A flow increase without increase in CMRO2

Page 45: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Calibrated BOLD for measuring CMRO2

Hoge R et al

CMRO2-CBF coupling:

slope ~2

Calibrated BOLD

Page 46: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

What else?

ASL

VASO

MRS

DWI

???

Page 47: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Neural Neural ResponseResponse

StimulusStimulus

CBVCBV

CBFCBF

CMROCMRO22

BOLDBOLD

Neurovascular Coupling

Page 48: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Arterial Spin Labeling

Williams et al. PNAS 1992

Relies on endogenous contrast agentMagnetically label water at the neck (below imaging plane)Labeled blood moves downstream and mixes with stationary tissue water

movement of blood water:

measure of CBF

CB

F (

ml g

-1 m

in-1)

pCO2 (mmHg)

Page 49: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

ASL: Tagging StrategiesUniversal concept: “tag” and “control”

tag image

Wait for tag blood water spins to arrive

tag delay: 500 - 2000 msec time

Page 50: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

ASL: Tagging StrategiesUniversal concept: “tag” and “control”

Wait the same amount of time but no tagging

no tag image

Page 51: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

ASL: Tagging StrategiesUniversal concept: “tag” and “control”

no tag image

Control image is important

same tag locationoff-resonance

global tag

Wait the same amount of time but no tagging

Page 52: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

A bit about baselines

hemodynamicresponse

Page 53: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Physiological baseline Baseline CBF,

But CBF CMRO2 unchanged (probably) (Brown et al JCBFM 2003)

BOLD response (probably)

Cohen et al JCBFM 2002

Page 54: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Implications

Factors altering baseline state Disease Sedation Anxiety Vasoactive medications

Global and local

CBF (ASL) may be more robust?

Page 55: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Noise sources

What is noise in a BOLD experiment? Unmodelled variation in

the time-series Intrinsic MRI noise

Independent of field strength, TE

Thermal noise from subject and RF coil

Physiological noise Increases with field

strength, depends on TE

Cardiac pulsations Respiratory motion

and B0 shift Vasomotion, 0.1Hz Blood gas fluctuations “Resting state”

networks Also

Scanner drift (heating up)

Page 56: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

At 3Tesla

Physiological noise >scanner + thermal noise

Physiological noise GM > Physiological noise WM

Page 57: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Spatial distribution of noise Motion at intensity boundaries

volunteer Respiratory B0 shift

Physiological noise in blood vessels and grey matter

Page 58: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Noise structure

1/f dependence BOLD is bad for detecting long time-scale activation

frequency

BOLD noise

Page 59: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Noise or signal?

Noise is unmodelled signal Spatially structured Temporally structured

“Physiological” signal Vascular properties

“Neuronal” signal Resting state networks Resting fluctuations Stimulus induced deactivation

Separation:all haemodynamic

Page 60: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Physiological noise

Motion McFLIRT correction

Cardiac Pulsations (aliased)

Respiratory Motion B0 shift

RETROICOR correction

Page 61: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Physiological signal

Low frequency haemodynamic oscillations Information about vascular properties CO2 reactivity

Autoregulation

• Is it a problem?• Can we use it?

Page 62: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

BOLD response to CO2

• CO2 is a potent vasodilator50

100

CB

F m

l/100

g/m

in

Normal

PaCO2

80604020 mmHg

CB

V m

l/100

g

4.05.0

3.0

Hypercapnia:

CBF, CBV [deoxyHb] T2* SBOLD

• Previous investigations use sustained hyper/hypocapnia challenges to investigate regional sensitivity (1.5T)

e.g. Posse et al. 1997, 2001, Rostrup et al. 2000

Page 63: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Spontaneous CO2 fluctuations

Resting PETCO2 PETCO2 power spectrum

• End-tidal CO2 (PETCO2) is a good measure of arterial CO2

• Fluctuations 0 - 0.05 Hz (Van den Aardweg & Karemaker, 2002)

• Overlaps with stimulus frequencies• Can correlate with stimulation

Wise et al Neuroimage 2004

Page 64: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

BOLD-CO2 (resting) correlation

r=0.5, Z=5.5

Page 65: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

What about 7T?

Page 66: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

FMRI at 7T

Page 67: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Bigger is better

High field = high SNR and high BOLD CNR

At higher magnetic fields, the short T2 of blood means that its signal is attenuated relative to that from tissue at the TE’s used for fMRI.

Hence it is expected that higher spatial specificity can be obtained in BOLD data acquired at high field as the intra-vascular signal contribution from draining veins is reduced

Page 68: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Pros and Cons

The increase in physiological noise can reduce the gains in BOLD CNR at ultra-high field

Higher BOLD signal means more signal drop-out

However, an increased BOLD CNR allows fMRI to be performed at higher spatial resolution, which has the potential advantage of reduced signal drop-out due to magnetic field inhomogeneities and longer baseline T2

At high resolution the effect of intrinsic noise can dominate that of physiological noise

Page 69: Functional MRI Daniel Bulte Centre for Functional Magnetic Resonance Imaging of the Brain University of Oxford

Extra Reading:

Buxton et al. Modeling the hemodynamic response to brain activation. NeuroImage 23 (2004) S220–S233

Raichle & Mintun. BrainWork and Brain Imaging. Annu. Rev. Neurosci. 2006. 29:449–76

http://www.fmrib.ox.ac.uk/Members/bulte/