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What are we measuring with M/EEG (and what are we measuring with) Gareth

Содержание

A brief historyThe EEG & MEG instrumentationNeuronal basis of the signalForward modelsOutline

Слайды и текст этой презентации

Слайд 1What are we measuring with M/EEG

(and what are we measuring

with)
Gareth Barnes
UCL
SPM Course – May 2012 – London

What are we measuring with M/EEG(and what are we measuring with)Gareth BarnesUCLSPM Course – May 2012 –

Слайд 2A brief history

The EEG & MEG instrumentation

Neuronal basis of the

signal

Forward models
Outline

A brief historyThe EEG & MEG instrumentationNeuronal basis of the signalForward modelsOutline

Слайд 3EEG history
1875: Richard Caton (1842-1926) measured currents inbetween the cortical

surface and the skull, in dogs and monkeys
1929: Hans Berger

(1873-1941) first EEG in humans (his young son), description of alpha and beta waves

1950s. Grey Walter ( 1910 – 1977). Invention of topographic EEG maps.

EEG history1875: Richard Caton (1842-1926) measured currents inbetween the cortical surface and the skull, in dogs and

Слайд 4MEG history
David
Cohen
1962: Josephson effect


1968: first (noisy) measure of a magnetic

brain signal [Cohen, Science 68]


1970: James Zimmerman invents the ‘Superconducting quantum interference device’

(SQUID)


1972: first (1 sensor) MEG recording based on SQUID [Cohen, Science 1972]


1973: Josephson wins the Nobel Prize in Physics
- And goes on to study paranormal activity…

Brian-David
Josephson

MEG historyDavidCohen1962: Josephson effect1968: first (noisy) measure of a magnetic brain signal [Cohen, Science 68]1970: James Zimmerman

Слайд 5
It is an ultrasensitive detector of magnetic flux.
It is made

up of a superconducting ring interrupted by one or two

Josephson Junctions.

Can measure field changes of the order of 10^-15 (femto) Tesla

(compare to the earth’s field of 10^-4 Tesla)

SQUIDS

It is an ultrasensitive detector of magnetic flux.It is made up of a superconducting ring interrupted by

Слайд 6There are different types of sensors
Magnetometers: measure the magnetic flux

through a single coil
Gradiometers: when more flux passes through the

lower coil (near the head) than the upper get a net change in current flow at the inut coil.

Flux transformers

There are different types of sensorsMagnetometers: measure the magnetic flux through a single coilGradiometers: when more flux

Слайд 8The EEG & MEG instrumentation
Sensors
(Pick up coil)
SQUIDs
MEG
- 269 °C

The EEG & MEG instrumentationSensors(Pick up coil)SQUIDsMEG- 269 °C

Слайд 9From a single neuron to a neuronal assembly/column
A single

active neuron is not sufficient. ~100,000 simultaneously active neurons are

needed to generate a measurable M/EEG signal.

Pyramidal cells are the main direct neuronal sources of EEG & MEG signals.

Synaptic currents but not action potentials generate EEG/MEG signals

What do we measure with EEG & MEG ?

From a single neuron to a neuronal assembly/column A single active neuron is not sufficient. ~100,000 simultaneously

Слайд 10Holmgren et al. 2003
Lateral connectivity
-local

Holmgren et al. 2003Lateral connectivity-local

Слайд 11Volume currents
Magnetic field
Electrical potential difference (EEG)
5-10nAm
Aggregate post-synaptic currents
of ~100,000

pyrammidal neurons
cortex
skull
scalp
MEG pick-up coil

Volume currentsMagnetic fieldElectrical potential difference (EEG)5-10nAmAggregate post-synaptic currents of ~100,000 pyrammidal neuronscortexskullscalpMEG pick-up coil

Слайд 12MEG
EEG
What do we measure with EEG & MEG ?
From a

single source to the sensor: MEG

MEGEEGWhat do we measure with EEG & MEG ?From a single source to the sensor: MEG

Слайд 13Fig. 14. Return currents for the left thalamic source on

a coronal cut through the isotropic model (top row) and

the model with 1:10 anisotropic white matter compartment (volume constraint, bottom row): the return current directions are indicated by the texture and the magnitude is color coded.

C.H. Wolters et al. / NeuroImage 30 (2006) 813– 826

Fig. 14. Return currents for the left thalamic source on a coronal cut through the isotropic model

Слайд 14Lead fields
MEG
EEG
Dipolar sources
Head tissues
(conductivity & geometry)
The forward problem

Lead fieldsMEGEEGDipolar sourcesHead tissues(conductivity & geometry)The forward problem

Слайд 15Different head models (lead field definitions) for the forward problem
Finite

Element

Boundary Element

Multiple Spheres

Single Sphere
Simpler
models

Different head models (lead field definitions) for the forward problemFinite ElementBoundary ElementMultiple SpheresSingle SphereSimplermodels

Слайд 16Can MEG see gyral sources ?
A perfectly radial source in

a spherical conductor
produces no external magnetic field.

Can MEG see gyral sources ?A perfectly radial source in a spherical conductorproduces no external magnetic field.

Слайд 17A quantitative assessment of the sensitivity of whole-head MEG to

activity in the adult human cortex. Arjan Hillebrand et al.

,
NeuroImage 2002

Source depth, rather than orientation, limits the sensitivity of MEG to electrical activity on the cortical surface. There are thin strips (approximately 2mm wide) of very poor resolvability at the crests of gyri, however these strips are abutted by elements with nominal tangential component yet high resolvability due to their proximity to the sensor array.

Can MEG see gyral sources ?

A quantitative assessment of the sensitivity of whole-head MEG to activity in the adult human cortex. Arjan

Слайд 18EEG Auditory Brainstem Response
Wave I/II (

or at entry to brainstem+ cochlear nucleus
Wave III. Ipsilateral cochlear

nucleus / superior olivary complex
Wave IV. Fibres leaving cochlear nucleus and/or superior olivary complex
Wave V. Lateral lemniscus


EEG Auditory Brainstem ResponseWave I/II (

Слайд 19
Volume 295, Issue 7654, 9 May 1970, Pages 976-979
IS

ALPHA RHYTHM AN ARTEFACT?
O. C. J. Lippold and G.

E. K. Novotny
Department of Physiology, University College, London, W.C.1, United Kingdon

Abstract
It is postulated that occipital alpha rhythm in man is not generated
in the occipital cortex, but by tremor of the extraocular muscles.
It is thought that tremor modulates the corneoretinal potential and
this modulation is recorded at the occiput because of the
anatomical organisation of the orbital contents within the skull.

Volume 295, Issue 7654, 9 May 1970, Pages 976-979   IS ALPHA RHYTHM AN ARTEFACT?

Слайд 20Summary
EEG is sensitive to deep (and radial) sources but a

very precise head model is required to get an accurate

picture of current flow.
MEG is relatively insensitive to deeper sources but forward model is simple.
SummaryEEG is sensitive to deep (and radial) sources but a very precise head model is required to

Слайд 21Supp_Motor_Area
Parietal_Sup
Frontal_Inf_Oper
Occipital_Mid
Frontal_Med_Orb
Calcarine
Heschl
Insula
Cingulum_Ant
ParaHippocampal
Hippocampus
Putamen
Amygdala
Caudate
Cingulum_Post
Brainstem
Thalamus
STN
Hung et al. 2010; Cornwell et al. 2007,

2008
Parkonen et al. 2009
Cornwell et al. 2008; Riggs et

al. 2009

RMS Lead field
Over subjects and voxels

Timmerman et al. 2003

MEG Sensitivity to depth

Supp_Motor_AreaParietal_SupFrontal_Inf_OperOccipital_MidFrontal_Med_OrbCalcarineHeschlInsula Cingulum_AntParaHippocampalHippocampusPutamenAmygdalaCaudateCingulum_PostBrainstemThalamusSTN Hung et al. 2010; Cornwell et al. 2007, 2008 Parkonen et al. 2009Cornwell et al.

Слайд 22
Sqrt(Trials)

sqrt(Noise Bandwidth)
400 Trials, 40Hz BW
200 Trials, 20 Hz BW
Sensitivity can

be improved by knowing signal of interest

Sqrt(Trials)sqrt(Noise Bandwidth)400 Trials, 40Hz BW200 Trials, 20 Hz BWSensitivity can be improved by knowing signal of interest

Слайд 24Forward problem
Lead fields
MEG
EEG
Dipolar sources
Lead fields
forward
model

Forward problemLead fieldsMEGEEGDipolar sourcesLead fieldsforwardmodel

Слайд 25Y = g()+ 
forward
model
MEG
The inverse problem
For example,
can make

a good guess
at realistic orientation
(along pyrammidal cell bodies,


perpendicular to cortex)

EEG

The inverse problem (estimating source activity from sensor data)
is ill-posed. So you have add some prior assumptions

Y = g()+  forwardmodelMEGThe inverse problemFor example, can make a good guess at realistic orientation (along

Слайд 26Summary

Measuring signals due to aggregate post-synaptic currents (modeled as dipoles)
Lead

fields are the predicted signal produced by a dipole of

unit amplitude.
MEG is limited by SNR. Higher SNR= resolution of deeper structures.
EEG is limited by head models. More accurate head models= more accurate reconstruction.

SummaryMeasuring signals due to aggregate post-synaptic currents (modeled as dipoles)Lead fields are the predicted signal produced by

Слайд 27Google Ngram viewer
Thanks to Laurence Hunt and Tim Behrens
Occurrence in

English language texts
EEG
fMRI
MEG

Google Ngram viewerThanks to Laurence Hunt and Tim BehrensOccurrence in English language textsEEGfMRIMEG

Слайд 28Logothetis 2003
Local Field Potential (LFP) / BOLD

Logothetis 2003Local Field Potential (LFP) / BOLD

Слайд 29Note that the huge dimensionality of the data allows you

to infer a lot more than source location.. (DCM talks

tomorrow)
For example, gamma frequency seems to relate to amount of GABA.

Muthukumaraswamy et al. 2009

Note that the huge dimensionality of the data allows you to infer a lot more than source

Слайд 30Jean Daunizeau
Karl Friston
James Kilner
Stefan Kiebel
Guillaume Flandin
Vladimir Litvak
Christophe Phillips
Rik Henson
Marta Garrido
Will

Penny
Rosalyn Moran
Jérémie Mattout

JM Schoffelen
Arjan Hillebrand

Jean DaunizeauKarl FristonJames KilnerStefan KiebelGuillaume FlandinVladimir LitvakChristophe PhillipsRik HensonMarta GarridoWill PennyRosalyn MoranJérémie MattoutJM SchoffelenArjan Hillebrand

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