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H O M E O S T A T I C C R I T I C A L I T Y
I N S T O C H A S T I C I N T E G R A T E -
A N D - F I R E N E U R O N S
O S A M E K I N O U C H I
P H Y S I C S D E P A R T M E N T - F F C L R P
S Ã O P A U L O U N I V E R S I T Y - B R A Z I L
B R A I N C R I T I C A L I T Y V I R T U A L W O R K S H O P
W E D N E S D A Y O C T O B E R 7 , 2 0 2 0
H O M E O S T A T I C C R I T I C A L I T Y =
S E L F - O R G A N I Z E D Q U A S I - C R I T I C A L I T Y ( S O Q C )
W I T H O U T I N F I N I T E S E P A R A T I O N O F T I M E S C A L E S
Three main homeostatic mechanisms:
• Homeostatic Synapses 𝑊!" 𝑡 :
𝑁𝐾 synaptic equations
• Homeostatic Neuronal Gains Γ![𝑡]:
𝑁 gain equations
• Homeostatic FiringThresholds 𝜃![𝑡]:
𝑁 threshold equations
H O M E O S T A T I C S Y N A P S E S
M E C H A N I S M S O F S E L F - O R G A N I Z E D
Q U A S I - C R I T I C A L I T Y I N N E U R O N A L N E T W O R K S M O D E L S
• Markran-Tsodyks (MT) model:
H O M E O S TAT I C S Y N A P S E S
• Levina-Hermann-Geisel (LHG) model (constant u):
D I S C R E T E T I M E ( L G H ) S Y N A P S E S
D I S C R E T E T I M E S T O C H A S T I C
I N T E G R A T E - A N D - F I R E N E U R O N
• 𝑠! ∈ 0,1 𝑖 = 1, ⋯ , 𝑁
• 𝑉! 𝑡 + 1 = 𝜇𝑉! 𝑡 + 𝐼! 𝑡 + ∑"
#
𝑊!" 𝑡 𝑠"[𝑡] if 𝑠! 𝑡 = 0
• 𝑉! 𝑡 + 1 = 0 if 𝑠! 𝑡 = 1
• 𝑃 𝑠! = 1 = Φ 𝑉𝑖
• 0 < 𝜇 < 1 = leakage parameter
• 𝐼! = external current
• 𝑊!" = synaptic weight
F I R I N G F U N C T I O N S ɸ ( V )
• Linear-saturating Φ 𝑉 :
• Φ 𝑉! = 0 if 𝑉! ≤ 𝜃!
• Φ 𝑉! = Γ 𝑉! − 𝜃! if 𝜃! < 𝑉! < 𝑉!
$
= 𝜃! + 1/Γ
• Φ 𝑉! = 1 if 𝑉! ≥ 𝑉!
$
• Rational Φ 𝑉! :
• Φ 𝑉! =
% &!'(!
)*% &!'(!
Θ 𝑉! − 𝜃!
θ VS
1
ɸ(V)
θ
ɸ(V)
1
𝚪
𝚪
M T A N D L H G D Y N A M I C S A R E S U F F I C I E N T
B U T N O T N E C E S S A RY M E C H A N I S M S
which has a form very similar to sandpile models if 1/𝛕 → 0, u → 0, u/𝛕 → 0
P R O P O S E D I N 1 9 9 8 B U T U N F O R T U N A T E L Y
N O T S T U D I E D . . .
Only N equations,
notice si , not sj
Stochastic oscillations and avalanches with homeostatic neuronal gain
𝑌 =
𝐼
𝜃
𝑔 =
𝑊!!
𝑊""
=
𝑊!!
𝐽
H O M E O S T A T I C S E T P O I N T : 𝑾 ∗ , 𝒉 ∗ = 𝑰 − ( 𝟏 − 𝝁 ) 𝜽 ∗
15
In the 𝑊, ℎ coordinates:
𝑊∗ = 𝑊" +
𝐴
1 + 𝜏# 𝑢#
ℎ∗
=
1
𝑐 𝜏$ 𝑢$
2
In the 𝑔, 𝑌 coordinates:
𝑔∗
=
𝑔"
1 + 1/(𝜏# 𝑢#)
+
𝑝 − 𝐴/𝐽
𝑞(1 + 𝜏# 𝑢#)
𝑌∗ = 𝑌" 1 −
1
𝑐𝐼𝜏$ 𝑢$
2
For large separation of time scales (𝜏#, 𝜏$ > 100 ms):
𝑊∗
, ℎ∗
, 𝑔∗
, 𝑌∗
→ 𝑊" , ℎ" , 𝑔" , 𝑌"
F I X E D P O I N T I S A F O C U S ( W H I T E B U L L E T ) C L O S E T O T H E
C R I T I C A L P O I N T ( R E D B U L L E T ) .
F I N I T E S I Z E N O I S E ( D E M O G R A P H I C N O I S E ) → T H E S Y S T E M
H O V E R S A R O U N D I T
16
Asynchronous
Irregular (AI)
Brunel (2000)
AI
17
Contact:
okinouchi@gmail.com
Ludmila BrochiniAriadne A. Costa Maurício Girardi-Schappo Tawan T. A. Carvalho Mauro Copelli

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Homeostatic criticality in stochastic integrate- and-fire neurons

  • 1. H O M E O S T A T I C C R I T I C A L I T Y I N S T O C H A S T I C I N T E G R A T E - A N D - F I R E N E U R O N S O S A M E K I N O U C H I P H Y S I C S D E P A R T M E N T - F F C L R P S Ã O P A U L O U N I V E R S I T Y - B R A Z I L B R A I N C R I T I C A L I T Y V I R T U A L W O R K S H O P W E D N E S D A Y O C T O B E R 7 , 2 0 2 0
  • 2. H O M E O S T A T I C C R I T I C A L I T Y = S E L F - O R G A N I Z E D Q U A S I - C R I T I C A L I T Y ( S O Q C ) W I T H O U T I N F I N I T E S E P A R A T I O N O F T I M E S C A L E S Three main homeostatic mechanisms: • Homeostatic Synapses 𝑊!" 𝑡 : 𝑁𝐾 synaptic equations • Homeostatic Neuronal Gains Γ![𝑡]: 𝑁 gain equations • Homeostatic FiringThresholds 𝜃![𝑡]: 𝑁 threshold equations
  • 3. H O M E O S T A T I C S Y N A P S E S M E C H A N I S M S O F S E L F - O R G A N I Z E D Q U A S I - C R I T I C A L I T Y I N N E U R O N A L N E T W O R K S M O D E L S • Markran-Tsodyks (MT) model:
  • 4. H O M E O S TAT I C S Y N A P S E S • Levina-Hermann-Geisel (LHG) model (constant u):
  • 5. D I S C R E T E T I M E ( L G H ) S Y N A P S E S
  • 6. D I S C R E T E T I M E S T O C H A S T I C I N T E G R A T E - A N D - F I R E N E U R O N • 𝑠! ∈ 0,1 𝑖 = 1, ⋯ , 𝑁 • 𝑉! 𝑡 + 1 = 𝜇𝑉! 𝑡 + 𝐼! 𝑡 + ∑" # 𝑊!" 𝑡 𝑠"[𝑡] if 𝑠! 𝑡 = 0 • 𝑉! 𝑡 + 1 = 0 if 𝑠! 𝑡 = 1 • 𝑃 𝑠! = 1 = Φ 𝑉𝑖 • 0 < 𝜇 < 1 = leakage parameter • 𝐼! = external current • 𝑊!" = synaptic weight
  • 7. F I R I N G F U N C T I O N S ɸ ( V ) • Linear-saturating Φ 𝑉 : • Φ 𝑉! = 0 if 𝑉! ≤ 𝜃! • Φ 𝑉! = Γ 𝑉! − 𝜃! if 𝜃! < 𝑉! < 𝑉! $ = 𝜃! + 1/Γ • Φ 𝑉! = 1 if 𝑉! ≥ 𝑉! $ • Rational Φ 𝑉! : • Φ 𝑉! = % &!'(! )*% &!'(! Θ 𝑉! − 𝜃! θ VS 1 ɸ(V) θ ɸ(V) 1 𝚪 𝚪
  • 8. M T A N D L H G D Y N A M I C S A R E S U F F I C I E N T B U T N O T N E C E S S A RY M E C H A N I S M S which has a form very similar to sandpile models if 1/𝛕 → 0, u → 0, u/𝛕 → 0
  • 9. P R O P O S E D I N 1 9 9 8 B U T U N F O R T U N A T E L Y N O T S T U D I E D . . .
  • 11. Stochastic oscillations and avalanches with homeostatic neuronal gain
  • 13.
  • 14.
  • 15. H O M E O S T A T I C S E T P O I N T : 𝑾 ∗ , 𝒉 ∗ = 𝑰 − ( 𝟏 − 𝝁 ) 𝜽 ∗ 15 In the 𝑊, ℎ coordinates: 𝑊∗ = 𝑊" + 𝐴 1 + 𝜏# 𝑢# ℎ∗ = 1 𝑐 𝜏$ 𝑢$ 2 In the 𝑔, 𝑌 coordinates: 𝑔∗ = 𝑔" 1 + 1/(𝜏# 𝑢#) + 𝑝 − 𝐴/𝐽 𝑞(1 + 𝜏# 𝑢#) 𝑌∗ = 𝑌" 1 − 1 𝑐𝐼𝜏$ 𝑢$ 2 For large separation of time scales (𝜏#, 𝜏$ > 100 ms): 𝑊∗ , ℎ∗ , 𝑔∗ , 𝑌∗ → 𝑊" , ℎ" , 𝑔" , 𝑌"
  • 16. F I X E D P O I N T I S A F O C U S ( W H I T E B U L L E T ) C L O S E T O T H E C R I T I C A L P O I N T ( R E D B U L L E T ) . F I N I T E S I Z E N O I S E ( D E M O G R A P H I C N O I S E ) → T H E S Y S T E M H O V E R S A R O U N D I T 16 Asynchronous Irregular (AI) Brunel (2000) AI
  • 17. 17 Contact: okinouchi@gmail.com Ludmila BrochiniAriadne A. Costa Maurício Girardi-Schappo Tawan T. A. Carvalho Mauro Copelli