modelling membrane potentials by diffusion leaky
play

Modelling Membrane Potentials by Diffusion Leaky Integrate-and-Fire - PowerPoint PPT Presentation

Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Modelling Membrane Potentials by Diffusion Leaky Integrate-and-Fire Models Patrick Jahn DEPARTMENT OF MATHEMATICAL SCIENCES UNIVERSITY OF


  1. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Modelling Membrane Potentials by Diffusion Leaky Integrate-and-Fire Models Patrick Jahn DEPARTMENT OF MATHEMATICAL SCIENCES UNIVERSITY OF COPENHAGEN jahn@math.ku.dk CIRM, Marseille - January 18, 2009 Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  2. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Contents 1 Diffusion Leaky Integrate-and-Fire Neuronal Models 2 Modelling Membrane Potentials in Motoneurons by time-inhomogeneous Diffusion Models Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  3. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Biological Background Figure: The Neuron Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  4. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Membrane Potential recorded by W. Kilb, Mainz −20 potential [mV] −30 −40 −50 0 1 2 3 4 5 6 time [s] Figure: This membrane potential was recorded in vitro from a pyramidal neuron belonging to cortical slice preparation of a juvenile C57bl/6 mouse. Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  5. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Diffusion Leaky Integrate-and-Fire Neuronal Model S x 0 . . . � �� � � �� � � �� � T 1 T 2 T n Assume the process X between spikes is a Diffusion process given by d X t = 1 τ ( a − X t ) d t + σ ( X t ) d B t Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  6. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Diffusion Leaky Integrate-and-Fire Neuronal Model S x 0 . . . � �� � � �� � � �� � T 1 T 2 T n Assume the process X between spikes is a Diffusion process given by d X t = 1 τ ( a − X t ) d t + σ ( X t ) d B t Goal: Estimate β ( · ) := 1 τ ( a − · ), σ ( · ), x 0 , S from discrete observations of X and from the observation of iid ISIs (level crossing times) T i , i = 1 , . . . , n . . Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  7. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Diffusion Leaky Integrate-and-Fire Neuronal Model S x 0 . . . � �� � � �� � � �� � T 1 T 2 T n Assume the process X between spikes is a Diffusion process given by d X t = 1 τ ( a − X t ) d t + σ ( X t ) d B t Goal: Estimate β ( · ) := 1 τ ( a − · ), σ ( · ), x 0 , S from discrete observations of X and from the observation of iid ISIs (level crossing times) T i , i = 1 , . . . , n . . Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  8. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Problem of Finding Excitation Threshold and Reset Value −46 −47 −48 potential [mV] −49 S ? −50 −51 x 0 ? −52 1.0 1.5 2.0 2.5 3.0 3.5 time [s] Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  9. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Problem of Finding Excitation Threshold and Reset Value 17Sept08_023.asc alle spikes uebereinanderlegen / spikezeiten auf 0 transformieren 0 −10 −20 [mV] −30 −40 −50 −0.04 −0.02 0.00 0.02 0.04 17Sept08_023.asc Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  10. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Strategy θ 2 θ 1 � �� � � �� � . . . � �� � T 1 T 2 T n 1. Fixing drift and diffusion coefficient with nonparametric methods proposed by R. H¨ opfner (2006). So assume X is given by d X t = 1 τ ( a − X t ) d t + σ ( X t ) d B t Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  11. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Strategy θ 2 θ 1 � �� � � �� � . . . � �� � T 1 T 2 T n 1. Fixing drift and diffusion coefficient with nonparametric methods proposed by R. H¨ opfner (2006). So assume X is given by d X t = 1 τ ( a − X t ) d t + σ ( X t ) d B t 2. Estimate θ 1 = x 0 and θ 2 = S from the observation of iid inter spike times � � t ≥ 0 | X ( θ 1 ) T i := inf = θ 2 , i = 1 , . . . , n . t Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  12. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Strategy θ 2 θ 1 � �� � � �� � . . . � �� � T 1 T 2 T n 1. Fixing drift and diffusion coefficient with nonparametric methods proposed by R. H¨ opfner (2006). So assume X is given by d X t = 1 τ ( a − X t ) d t + σ ( X t ) d B t 2. Estimate θ 1 = x 0 and θ 2 = S from the observation of iid inter spike times � � t ≥ 0 | X ( θ 1 ) T i := inf = θ 2 , i = 1 , . . . , n . t Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  13. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Some Facts. . . In the most famous cases, where X is an Ornstein-Uhlenbeck (OU) or a Cox-Ingersoll-Ross (CIR) process, no explicit expression for the density of the level crossing time T is known. However, we know its Laplace transfrom (LT) as a ratio of special functions. (Jahn, PhD-Thesis 2009): For the OU and CIR cases the estimation problem of θ 1 = x 0 and θ 2 = S was solved by using Millar’s framework (1984) for minimum distance estimators via the comparison of empirical and theoretical LT with respect to a suitable Hilbert space norm . . . . Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  14. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models Some Facts. . . In the most famous cases, where X is an Ornstein-Uhlenbeck (OU) or a Cox-Ingersoll-Ross (CIR) process, no explicit expression for the density of the level crossing time T is known. However, we know its Laplace transfrom (LT) as a ratio of special functions. (Jahn, PhD-Thesis 2009): For the OU and CIR cases the estimation problem of θ 1 = x 0 and θ 2 = S was solved by using Millar’s framework (1984) for minimum distance estimators via the comparison of empirical and theoretical LT with respect to a suitable Hilbert space norm . . . . Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  15. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models The Minimum Distance Estimator w.r.t. the LT Theorem (J. 2009) Let X be an OU or a CIR process. Define the empirical LT of the level crossing time T of X from θ 1 to θ 2 and the corresponding family of possibly true LTs by n � L n ( α ) := 1 ˆ e − α T i L θ ( α ) := E θ [ e − α T ] , and n i =1 then the MDE w.r.t. the LT θ 1 <θ 2 � ˆ θ ∗ n := arg inf L n − L θ � H is strongly consistent and asymptotically normal . Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  16. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models The Pearson Diffusion Case (work with Jesper L. Pedersen. . . ) Pearson Diffusion � ( X t − c ) 2 + d d B t , d X t = 1 τ ( a − X t ) d t + σ X 0 = θ 1 ≥ 0 Jesper computed the Laplace transform of T : E θ [ e − α T ] = g Re ( θ 1 , α ) − K ( α ) · h Re ( θ 1 , α ) g Re ( θ 2 , α ) − K ( α ) · h Re ( θ 2 , α ) where g , h and K are expressions of hypergemetric functions where the parameters of the diffusion X enter. Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  17. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models The Pearson Diffusion Case (work with Jesper L. Pedersen. . . ) Pearson Diffusion � ( X t − c ) 2 + d d B t , d X t = 1 τ ( a − X t ) d t + σ X 0 = θ 1 ≥ 0 Jesper computed the Laplace transform of T : E θ [ e − α T ] = g Re ( θ 1 , α ) − K ( α ) · h Re ( θ 1 , α ) g Re ( θ 2 , α ) − K ( α ) · h Re ( θ 2 , α ) where g , h and K are expressions of hypergemetric functions where the parameters of the diffusion X enter. Goal: Solve the identifiability problem and apply the developed Framework to this case... Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

  18. Diffusion Leaky Integrate-and-Fire Neuronal Models Modelling by time-inhomogeneous Diffusion Models The Pearson Diffusion Case (work with Jesper L. Pedersen. . . ) Pearson Diffusion � ( X t − c ) 2 + d d B t , d X t = 1 τ ( a − X t ) d t + σ X 0 = θ 1 ≥ 0 Jesper computed the Laplace transform of T : E θ [ e − α T ] = g Re ( θ 1 , α ) − K ( α ) · h Re ( θ 1 , α ) g Re ( θ 2 , α ) − K ( α ) · h Re ( θ 2 , α ) where g , h and K are expressions of hypergemetric functions where the parameters of the diffusion X enter. Goal: Solve the identifiability problem and apply the developed Framework to this case... Patrick Jahn - jahn@math.ku.dk Leaky Integrate-and-Fire Models

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend