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Which cellular mechanism yields compatibility between brain states, synaptic plasticity and neuromodulation?

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(1)

Mimic change in cell

size or cellular variability

Switch in brain states

can be global and long-lasting

or fast and localized

Synaptic plasticity

CONTEXT

How can switches in brain states

be compatible

with synaptic plasticity?

2sec

20 m

V

Tonic Discharge

nRt

Relay

2sec

20 m

V

EEG

Py ra m id al c el l

Up States

gamma

Models

We compare 6 conductance-based models of thalamic neurons

- with similar number of nb. of ionic currents

- different T-type calcium dynamics (I

CaT

)

C

m

̇V

m

= - I

Na

- I

K

-

I

CaT

- I

others

+ I

app

I

CaT

= g

CaT

m

α

CaT

h

CaT

(V - V

CaT

)

Slow activation of CaT channels (m

CaT

)

Instant. activation of CaT channels

C

m

Cm

0.1Cm

10Cm

Cellular level

I

app

experiment

Change in C

m

Is the model still switching?

0.01Cm

Which cellular mechanism yields compatibility

between brain states, synaptic plasticity and neuromodulation ?

Kathleen Coutisse and Guillaume Drion |

Department of Electrical Engineering and Computer Science, University of Liege, Liege, Belgium

B55

554.17

Restoring the slow mCaT

brings back the robustness

C

m

/5

Rhythmic network

Wrong transition

E

I

Syn. Plast.

Nmod

I

app

Network level

2-cell Network

Broader range of C

m

values is

covered by models with slow

calcium channel activation.

Intrinsic conductances

g

Na

, g

K

, g

CaT

, g

others

Synaptic conductances

g

AMPA

g

GABAa

g

GABAb

Mimic both mechanisms by adding

variability on nominal conductances

#

g [(1 − γ)g; 1 + γ g]

Study effect of neuromodulation and

synaptic plasticity on rhythm switches

EXPERIMENT

- Run each model for 1000 sets of param

100 % Homogeneity

10s

EXPERIMENT

20 % Heterogeinity

E

I

E

I

E

I

5Hz

0Hz

LFP activity of A 200-cell Network

1 2

3

4

5’

Models

Activation kinetics of T-type calcium channels

Slow-wave sleep Waking

Summary

Synaptic Plasticity

g

1

g

2

g

3

+50%

-50%

+50%

-50%

-50%

+50%

𝑔

𝑔

E

I

I

app

g

1

=g

Na

, g

2

= g

K

, g

3

= g

CaT

Run each model with slow activation

for 1000 sets (g

1

,g

2

,g

3

)

Check how many networks are switching.

Repeat for different kinetics of activation

g

1

g

2

g

3

+50%

-50%

+50%

-50%

-50%

+50%

𝑔

𝑔

E

I

Syn. Plast.

I

app

g

1

=g

AMPA

, g

2

= g

GABAa

, g

3

= g

GABAb

Neuromodulation

Experiment

T-type calcium channel opens slowly.

- Check how many networks are switching

References

A

Neurotransmitter

Postsynaptic receptor

Postsynaptic terminal

Frontiers in Synaptic Neuroscience www.frontiersin.org June 2010 | Volume 2 | Article 19 | 4

Froemke et al. Temporal modulation of STDP

the exponential function, respectively (Song et al., 2000; Bi and Poo, 2001; Froemke and Dan, 2002; Figures 1 and 2). Biologically,

STDP is unlikely to be a true single exponential process, but these exponential fits are a convenient way to adequately formalize STDP using a low parameter model.

Here we refer to this formulation of STDP, in which only the intervals between each pre/post pairing are considered for determi-nation of net synaptic modification, as the “history-independent” model. While sometimes found to be satisfactory when overall spike rates are relatively low ( 10 Hz), in general the history-independ-ent model provides poor estimates of the effects of more complex spike trains, even when one additional spike is added to a pre/post pair, i.e., using spike triplets instead of spike pairs to induce STDP (Pfister and Gerstner, 2006). Comparisons between the predicted and actual effects of spike trains on synaptic strength show that the predictions of the independent model are generally poor and STDP induction seems to be somewhat sensitive to technical

details, in terms of spike number, spike timing, spike frequency, and underlying mechanisms such as inhibitory regulation. This seems especially true for CA1 pyramidal cells in hippocampal slices, where it remains controversial what is minimally required for LTP and LTD (Pike et al., 1999; Nishiyama et al. 2000; Meredith et al., 2003; Wittenberg and Wang, 2006; Buchanan and Mellor, 2007; but see Campanac and Debanne, 2008).

This millisecond-scale time window for pre/post pairings to induce LTP or LTD forms the basis of the STDP learning rule for a given synaptic connection. To quantify the effect of pre/post pair-ing more precisely, both the pre post and post pre data can be fitted with single exponential functions: w=Ae| t|/, where

w is the percentage change in synaptic weight, t is the pre/post

spike interval, and A and are two free parameters found by fit-ting the data, represenfit-ting the scaling factor and time constant of

A B

FIGURE 2 | Pre/post pairing induces STDP at hippocampal and neocortical synapses. (A) STDP induced at CA3-CA3 synapses in

hippocampal slice cultures. Top, LTP induced by pre post pairing ( t = 15 ms). Center, LTD induced by post pre spiking ( t = -70 ms). Bottom, time window

for pre/post pairing to induce synaptic modifications. From Debanne et al. (1998). (B) As in A, but for layer 2/3 connections in acute brain slices of young rat visual cortex. From Froemke and Dan (2002) and Froemke et al. (2006).

No

rm

. E

PS

P

slo

pe

(%

)

Spike timing (msec)

neuromodulators

STN rec

ording

Down States

Presynaptic

Terminal

Connections between neurons change over time

property associated with

learning

STN (subthalamic nucleus) neurons change

neuronal rhythm when DBS is applied.

Models #

E

I

I

app

E

I

E

I

I

app

10Hz

0Hz

Models

Na activation

CaT inactivation

A

B

C

D

Drion et al. 2018

Destexhe et al. 1996

Destexhe et al.1998

Huguenard

&

McCormick 1992

Wang + slow m

CaT

Rush + slow m

CaT

Wang 1994

Rush1994

1 2

3

5 6

5 6

1

2

3

4

5

6

𝜏

1

234

/3

B

𝜏

1

234

/2

C

𝜏

1

234

D

𝜏

1

234

𝑥2

Norm( )

𝑔

Rh

yt

hm

ic

ne

tw

or

k

(%

)

0

100

Rh

yt

hm

ic

ne

tw

or

k

(%

)

0

100

0

100

0

100

Parameter set repartition

ü

ü

ü

CaT channel activation

Ultraslow

𝜏

Fast

1

93

𝜏

1

234

𝜏

:

234

Ultraslow

𝜏

Fast

1

93

𝜏

1

234

𝜏

:

234

Ultraslow

𝜏

Fast

1

93

𝜏

1

234

𝜏

:

234

𝜏

Fast

1

93

𝜏

1

234

Ultraslow

𝜏

:

234

Fast

Ultraslow

Nmod

Zagha, McCormick. 2017

Hammond et al. 2007

Froemke et al. 2006

Franci A., Drion G., Sepulchre R. 2018.

Drion G., Franci A., Seutin V., Sepulchre, R. 2012.

Contact

kathleen.coutisse@uliege.be

gdrion@uliege.be

Relative intrinsic variability

Rh

yt

hm

ic

ne

tw

or

k

(%

)

0

80

100

60

40

20

10% 20% 30%

1

2

3

5

6

1

Model

Models

Hyperpolarization switches the mean field rhythm of the uniform

population resulting in a high power band in the spectrogram.

In our brain, a population of neurons is very heterogeneous.

Only models with slow activation maintain the switch in rhythm.

Respect physiological time-scales

of channel kinetics

Modeling switches in brain states compatible

with synaptic plasticity and neuromodulation

relies on a slow calcium current activation.

Computational applications

Transcritical hybrid model

̇V = V

<

− w

<

+ I

̇w = ε(aV − w + w

A

)

Models without this cellular property

are fragile to change in parameters.

I

app

5

4

6

1

2

2

5'

6'

5

6

'

'

'

'

5sec

γ

'

'

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