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School on Modelling, Automation and Control of
Physiological variables
at the Faculty of Science,
University of Porto
2 -3 May, 2007
Topics on Biomedical Systems Modelling:
Normal brain rhythms and the transition to
epileptic activity
Fernando Lopes da Silva
Center of Neuroscience
Swammerdam Institute for Life Sciences
University of Amsterdam
Normal brain rhythms and the
transition to epileptic activity
The case of the brain rhythm in the alpha (8 -12 Hz) frequency range appearing over the
somatosensory cortex:
the mu rhythm
One interesting
property of the
Alpha rhythm of
the somato-
sensory cortex
(Mu rhythm) is
that it is
modulated by
movements of
the hands:
It is attenuated,
desynchronized
alpha (ERD), by
moving the
hands, and it is
enhanced at rest
(synchronized
alpha or ERS)
Power changes in
the Apha (Mu
rhythm) and Beta
frequency ranges
ERD and ERS
Depending on
whether the hand or
the foot is moved,
the spatio-temporal
pattern differs;
the patterns of both
conditions appear
as mirror images.
Normal brain rhythms and the
transition to epileptic activity
Two questions put to the theoreticians or modelers:
1. How is the Alpha rhythmic activity generated?
2. How can the mirror images of the spatio-temporalpatterns of ERD/ERS associated with hand or
foot movements be accounted for?
Basic neuronal network responsible for
rhythmic activities in
thalamo-cortical circuits
Steriade 1999
Normal brain rhythms and the
transition to epileptic activity
Computational model of the thalamo-
cortical neuronal networks
Time evolution of the
neuronal membrane
potential:
Synaptic currents
Synaptic conductances
are modeled by
convolving firing rate
frequency with synaptic
impulse response
Nonlinear GABA-B
synaptic response
Nonlinearity is realized
by a sigmoidal
function of the form:
Basic equations of the model (1)
The model was realized using the Simulink toolbox of Math Works. Simulations
were run using the ode3 integration method with a time step of 1 millisecond
duration. Postprocessing was done using Matlab.
Transfer between
firing rate and
membrane potential
Transfer function for
the burst firing mode
Where GB is the maximal firing rate within a burst, variables ninf(V) and
minf(V) are static sigmoidal functions that describe the fractions of
neurons that are deinactivated or activated, respectively. Expressions (9)
and (10) describe the time delay of IT inactivation.
Basic equations of the model (2)
Model
scheme
© SEIN, 2003
pyramidal cells
population
thalamocortical cells
population
interneuronal
population
thalamic RE cells
population
external inputs
burst generation
process
This result is an answer to question # 1:
How is the Alpha rhythmic activity generated?
Normal brain rhythms and the
transition to epileptic activity
But we have to consider also the second question:
2. How can the mirror images of the spatio-
temporal patterns of ERD/ERS associated with
hand or foot movements be accounted for?
Thalamocortical network
© SEIN, 2003Medical Physics Department
Extracellular activity of a RE neuron (yellow) and
cortical field potential (green) recorded in the
GAERS during a spike and wave discharge
downloaded from Crunelli Research Group:
www. thalamus.org.uk
pyramidal cell
GABAergic interneuron
thalamic reticular (RE) neuron
thalamocortical (TC) neuron
In both TC and RE cells
burst firing is provided
by IT calcium current
Thalamic
ReticularNucleus
Thalamo-corticalRelayNucleus
Excitation Inhibition
This result means that the mechanism of recurrent inhibition between
neighboring thalamo-cortical modules can account for the mirror images of the
spatio-temporal patterns of ERD/ERS elicited by hand or foot movements,
respectively.
ERD
ERS
Normal brain rhythms and the
transition to epileptic activity
• How can this transition to epileptic
activity take place?
How does the transition to “epileptic
activity” take place?
We have to examine how this occurs in
patients and in animal models
EEG and
Video
during an
epileptic
absence
(“petit
mal”)
! genetic model.
! no neurological defects.
! absences are characterized by behavioral arrest and spike and
wave discharges (SWDs) in the EEG.
! pharmacological responses is similar to that of patients with
absences.
The WAG/Rij rat as model for absences seizures
(Gilles van Luijtelaar and Ton Coenen)
Spontaneousabsence:
Patient isrequested topress a buttonimmediately aftera technician didthe same.
Normal brain rhythms and the
transition to epileptic activity
• This is likely to be due to the fact that these neuronal
networks are complex non-linear systems:
• Such networks may display complex dynamics with
more than one stable state; in this case:
• These observations indicate that neuronal networks
can display qualitatively different dynamical states.
" A normal “on-going steady-state”, and
" An “oscillatory epileptiform, or paroxysmal state”.
This is what happens in epilepsy.
Ca 2+ T-channel
GABA
A & BComputer model
of a thalamo-
cortical network
capable of
displaying a
bifurcation
betweem two
states, (i) a
normal
oscillatory state,
and (ii) a
paroxystic
seizure state.
Simulation example
Simulated epoch
Power spectra
Spindle - rat
On-going state- model
Paroxysm - rat
Paroxysmal state - model
two stable statesThis is evidence for bi-stability: one network
Example
of a
bifurcation
between
two states:
“normal”
&
“seizure”
(absence
type),
both in
the model
and in
EEG real
signals.
Sensitivity of the Model to a set of parameters
Occurrence of transition to “epileptic
seizure” mode: parameter sensitivity
Phase portraits of the system under non
epileptic and epileptic conditions
Normal brain rhythms and the
transition to epileptic activity
" One prediction is that for this kind of seizures the
transition occurs randomly;
" A second prediction is that it should be possible to
stimulate the system in such a way that the transition
to the “seizure mode” may be aborted. This implies
that it should be possible to control the system’s
behavior.
What are the predictions of the model with respect to
the dynamics of absence seizures?
Normal brain rhythms and the
transition to epileptic activity
• The 1st prediction was tested by calculating
the distributions of durations and of intervals
inter-paroxysms.
Distribution of Durations
either of paroxysmal events or of inter-
paroxysmal events
© SEIN, 2003Medical Physics Department
Probability of termination in
unit time : p
Probability of survival of unit
time : 1- p
Process duration
Nu
mb
er o
f p
roce
sses
Exponential distribution
of process durations
P(t) = (1-p)(1-p)….(1-p)p
1 - p = e-! ! p = 1 - e-!
P(t) = (1 - e-!)e-!t
e-! " 1 - !
P(t) = !e-!t
Termination of a process
is random in time with
constant probability
simple calculation
In common language:
In math language:
0 10 20 30 40 50 60 70 80 90 1000
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
!e-!t
log
time
Prediction
Distributions of epochs duration - comparison of
simulated and rat (WAG/Rij) experimental data
© SEIN, 2003Medical Physics Department
Quasi- exponential (a ~ 1) distribution of
SWDs in rat (WAG/Rij)
Quasi-exponential distribution of duration of 3
Hz paroxysms in a patient with absence non-
convulsive seizures during the night
Normal brain rhythms and the
transition to epileptic activity
But ….
Does it hold in all similar cases?
Not exactly….
Gamma distribution of SWDs duration of
GAER rats
Normal brain rhythms and the
transition to epileptic activity
Thus, what do we have to modify in the
model?
It is necessary to include a ‘use-dependent
parameter’, i.e. a parameter that changes as a
seizure progresses.
New hypothesis to be tested:
K+ accumulation occurs in the course of SWD in glial
cells affecting the excitability of neurons.
,
!" /1 xeCxy##
=
!" /1 xeCxy##
=
Normal brain rhythms and the
transition to epileptic activity
Real EEG signals
Neuronal networks
Models/Simulated EEGs Statistics/
Dynamics
Signal analysis
Statistics/
Dynamics
Normal brain rhythms and the
transition to epileptic activity
The second prediction is that it should be
possible to control the occurrence or the
evolution of a seizure by means of counter-
stimulation.
Indeed in bistable systems a limit cycle may
be annihilated by a perturbation applied at the
appropriate time.
Counter-stimulation is capable of annihilating the
transition to the paroxysmal oscillation
Negative
stimulus
Positive
stimulus
Normal brain rhythms and the
transition to epileptic activityCollaborators from the Institute of Epilepsy SEIN (“Meer en
Bosch”, Heemstede) and MEG Center (Free University,
Amsterdam):
Stiliyan Kalitzin,
Piotr Suffczynski
Jaime Parra.
Dimitri Velis.
Wouter Blanes.
Elan Ohayon
Fernando Lopes da Silva
Suffczynski P, Lopes da Silva FH, Parra J, Velis DN, Bouwman BM, van Rijn CM,
van Hese P, Boon P, Khosravani H, Derchansky M, Carlen P, Kalitzin S. Dynamics
of epileptic phenomena determined from statistics of ictal transitions. IEEE Trans
Biomed Eng. 2006 Mar;53(3):524-32.
Suffczynski P, Lopes da Silva F, Parra J, Velis D, Kalitzin S. Epileptic transitions:
model predictions and experimental validation. J Clin Neurophysiol. 2005
Oct;22(5):288-99.
Suffczynski P, Kalitzin S, Lopes da Silva FH. Dynamics of non-convulsive
epileptic phenomena modeled by a bistable neuronal network. Neuroscience.
2004;126(2):467-84.
Lopes da Silva F, Blanes W, Kalitzin SN, Parra J, Suffczynski P, Velis DN.
Epilepsies as dynamical diseases of brain systems: basic models of the transition
between normal and epileptic activity. Epilepsia. 2003;44 Suppl 12:72-83.
Lopes da Silva FH, Blanes W, Kalitzin SN, Parra J, Suffczynski P, Velis DN.
Dynamical diseases of brain systems: different routes to epileptic seizures. IEEE
Trans Biomed Eng. 2003 May;50(5):540-8.
Suffczynski P, Kalitzin S, Pfurtscheller G, Lopes da Silva FH. Computational
model of thalamo-cortical networks: dynamical control of alpha rhythms in
relation to focal attention. Int J Psychophysiol. 2001 Dec;43(1):25-40.
Thalamo-cortical networks possess bi-stability. In Phase-space:
the normal steady-state is within the separatrix ( ),
the complex oscillatory (paroxysmal) state is outside.
Phase-space