MEG recording of brain signals

Preview:

Citation preview

400 fT1.0 s

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.1

MEG introductionBrain Signals

MEG seminarOct 06 2011

Bernhard Ross

Rotman Research Institute

Department of Medical BiophysicsUniversity of Toronto

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.2

Brain signals recorded with EEG and MEG

Understanding the neural mechanism underlying the EEG/MEGsignal and knowing about the possibilities and limitations of themethods has a large impact on design and performance of asuccessful study.

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.3

The origin of the neuroelectric / neuromagnetic signal

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.3

The origin of the neuroelectric / neuromagnetic signal

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.3

The origin of the neuroelectric / neuromagnetic signal

Ramon y Cajal

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.3

The origin of the neuroelectric / neuromagnetic signal

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.4

Intra-cellular current flow

Transmembrane current flowIntracellular current flowExtracellular current flow

The intracellular currentflow generates anexternalelectromagnetic field

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.5

Source activity: The dipole moment

6

?

dlAA��

I

Dipolemoment:q = I · dl

(Am, nAm)

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.5

Source activity: The dipole moment

6

?

dlAA��

I

Dipolemoment:q = I · dl

(Am, nAm)

Dipole moment of asingle neuron:0.2 . . . 0.5 pAme.g.:I=0.5nA, dl=1mm

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.5

Source activity: The dipole moment

6

?

dlAA��

I

Dipolemoment:q = I · dl

(Am, nAm)

AA��

n · I

Dipolemoment:q = n · I · dl

Dipole moment of asingle neuron:0.2 . . . 0.5 pAme.g.:I=0.5nA, dl=1mm

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.5

Source activity: The dipole moment

6

?

dlAA��

I

Dipolemoment:q = I · dl

(Am, nAm)

AA��

n · I

Dipolemoment:q = n · I · dl

Dipole moment of asingle neuron:0.2 . . . 0.5 pAme.g.:I=0.5nA, dl=1mmMEG/EEG evokedresponse:1 . . . 100 nAmn=2000 . . . 500,000synchronously activeneurons

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.6

Source of the MEG: – Anatomical organization in columnar structures

FROM: Hutsler and Galuske Trends in Neuroscience, 2003, 26:429-435

Neurons in the neocortex are organized in a hierarchy of micro-and macro-columns.

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.7

The neural columns are aligned perpendicular to the cortical surface

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.8

Coil configuration: first order gradiometer

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.9

Whole head MEG system

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.10

Not all sources appear equally in the MEG

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.10

Not all sources appear equally in the MEG

A dipole tangential to the skull produces astrong magnetic field outside the head.

A radial source may be missed in the MEG

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.11

The human magnetoencephalogram

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.12

The averaged auditory evoked response

0 200 400 600 800 1000Time (ms)

1

2

3

4

5

6

7

single trial data

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.12

The averaged auditory evoked response

0 200 400 600 800 1000Time (ms)

1

2

3

4

5

6

7

single trial data

0 200 400 600 800 1000Time (ms)

n=1

averaged data

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.12

The averaged auditory evoked response

0 200 400 600 800 1000Time (ms)

1

2

3

4

5

6

7

single trial data

0 200 400 600 800 1000Time (ms)

n=2

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.12

The averaged auditory evoked response

0 200 400 600 800 1000Time (ms)

1

2

3

4

5

6

7

single trial data

0 200 400 600 800 1000Time (ms)

n=4

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.12

The averaged auditory evoked response

0 200 400 600 800 1000Time (ms)

1

2

3

4

5

6

7

single trial data

0 200 400 600 800 1000Time (ms)

n=8

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.12

The averaged auditory evoked response

0 200 400 600 800 1000Time (ms)

1

2

3

4

5

6

7

single trial data

0 200 400 600 800 1000Time (ms)

n=16

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.12

The averaged auditory evoked response

0 200 400 600 800 1000Time (ms)

1

2

3

4

5

6

7

single trial data

0 200 400 600 800 1000Time (ms)

n=32

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.12

The averaged auditory evoked response

0 200 400 600 800 1000Time (ms)

1

2

3

4

5

6

7

single trial data

0 200 400 600 800 1000Time (ms)

n=64

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.12

The averaged auditory evoked response

0 200 400 600 800 1000Time (ms)

1

2

3

4

5

6

7

single trial data

0 200 400 600 800 1000Time (ms)

n=128

P1

N1

P2

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.13

Magnetic field waveforms of auditory evoked responses

600 fT

700 ms

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.13

Magnetic field waveforms of auditory evoked responses

600 fT

700 ms−200

−100

0

100

200

300

fT

−200

−100

0

100

200

300

0.0 0.2 0.4 0.6 0.8 1.0

sec

fT

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.14

Auditory evoked responses

-cortical responses

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.15

Why do we have positive and negative response components?

FROM: Niedermeyer and Lopes da Silva

Two factors decide about the polarity of the response:1. The nature of synaptic connection: excitatory or inhibitory.2. The location of synaptic contact: apical or basal.

Generally, subsequent waves are generated in different micro circuits.

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.16

Event related responses

Early responses are strictly time-locked to the stimulus (exogenouscomponents)

Later responses are time-locked to internal processing (endogenouscomponents)

trade off around 250 ms (?)

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.17

The first human MEG recording

David Cohen, Jim Zimmerman, MIT, 1971single channel SQUID sensor

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.17

The first human MEG recording

David Cohen, Jim Zimmerman, MIT, 1971single channel SQUID sensor

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.17

The first human MEG recording

David Cohen, Jim Zimmerman, MIT, 1971single channel SQUID sensor

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.17

The first human MEG recording

David Cohen, Jim Zimmerman, MIT, 1971single channel SQUID sensor

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.17

The first human MEG recording

David Cohen, Jim Zimmerman, MIT, 1971single channel SQUID sensor

Hans Berger, 1929

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.17

The first human MEG recording

David Cohen, Jim Zimmerman, MIT, 1971single channel SQUID sensor

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.18

Beta oscillations 15-30 Hz

Beta oscillations have been first observed in the motor system.

Beta increased during preparation for a movement.

Beta decreased at initiation of the movement.

and beta increased again at the end of the movement

Beta oscillations are involved in sensorimotor integration

Modulation of beta oscillation have been found in the auditory andvisual system.

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.19

Gamma oscillations 30-80 Hz

Gamma oscillation have been first observed as a short burst afterstimulus onset in the visual modality - also with auditory andsomatosensory stimulation.

There is a large interest in gamma oscillation because of a strongtheoretical framework related to feature binding, attention,consciousness ...

Gamma oscillations always increase in the active state

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.20

The micro circuit underlying gamma oscillations

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.21

early gamma oscillation aretime (phase) locked to thestimulus and can be detectedin the averaged sgnal

Endogenous gammaoscillations are less strictlytime (phase) locked to thestimulus. The signal iscanceled out in the average.

Instead we can analyze theevent related changes in themagnitude of oscillation.

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.22

Event related changes in oscillatory activity

-12-6 0 6 12

Time (s)

θ

-0.5 0 0.5 1 1.5 2

Time (s)

3 4 5 6 7 8

-3

0

8

10

12

14

-2

0

2

Sig

nal P

ow

er

Change (

dB

)

Fre

quency (

Hz)

β

16

20

24

28

Fre

quency (

Hz) -2

0

2γ1

30

40

50

-2

0

2

γ2 80

100

120

Time-frequencyanalysis of the MEGsignal

Change in signalstrength relative to aninactive pre-stimulusinterval

The signal changesare often termed’Event relatedsynchronisation (ERS)’and ’Event relateddesynchronisation(ERD)’

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.23

Synchrony between gamma oscillations

-100

-50

0

50

100

-0.4 -0.2 0 0.2 0.4 0.6 0.8 1

Sour

ce S

treng

th (n

Am)

Time (s)

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.23

Synchrony between gamma oscillations

-100

-50

0

50

100

-0.4 -0.2 0 0.2 0.4 0.6 0.8 1

Sour

ce S

treng

th (n

Am)

Time (s)

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.23

Synchrony between gamma oscillations

-20

-10

0

10

20

-0.4 -0.2 0 0.2 0.4 0.6 0.8 1

Sour

ce S

treng

th (n

Am)

Time (s)

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.23

Synchrony between gamma oscillations

-30

-20

-10

0

10

-0.4 -0.2 0 0.2 0.4 0.6 0.8 1

Sour

ce S

treng

th (n

Am)

Time (s)

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.23

Synchrony between gamma oscillations

-20

-10

0

10

20

-0.4 -0.2 0 0.2 0.4 0.6 0.8 1

Sour

ce S

treng

th (n

Am)

Time (s)

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.23

Synchrony between gamma oscillations

-10

0

10

-0.4 -0.2 0 0.2 0.4 0.6 0.8 1

-10

0

10

-0.4 -0.2 0 0.2 0.4 0.6 0.8 1

Sou

rce

Stre

ngth

(nA

m)

-10

0

10

-0.4 -0.2 0 0.2 0.4 0.6 0.8 1

Sou

rce

Stre

ngth

(nA

m)

-10

0

10

0.4 0.5 0.6 0.7

Sou

rce

Stre

ngth

(nA

m)

Time (s)

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.23

Synchrony between gamma oscillations

-10

0

10

-0.4 -0.2 0 0.2 0.4 0.6 0.8 1

-10

0

10

-0.4 -0.2 0 0.2 0.4 0.6 0.8 1

Sou

rce

Stre

ngth

(nA

m)

-10

0

10

-0.4 -0.2 0 0.2 0.4 0.6 0.8 1

Sou

rce

Stre

ngth

(nA

m)

-10

0

10

-0.2 -0.1 0 0.1

Sou

rce

Stre

ngth

(nA

m)

Time (s)

-6pt-6pt MEG

-2pt-2pt Bernhard Ross

1.24

Analysis of oscillatory activity

Phase locked responses (averaging, phase statistics)Event related changes in signal magnitude (ERS, ERD)Coherence between sensor signals and between source signalsEvent related changes in coherenceAnalysis of coupling between frequency bands (gamma - theta)Steady-state approaches

Recommended