\documentclass[a4paper,12pt,pdftex]{exam} \newcommand{\ptitle}{Integrate-and-fire neuron} \input{../header.tex} \firstpagefooter{Supervisor: Jan Benda}{phone: 29 74573}% {email: jan.benda@uni-tuebingen.de} \begin{document} \input{../instructions.tex} %%%%%%%%%%%%%% Questions %%%%%%%%%%%%%%%%%%%%%%%%% \begin{questions} \question The temporal evolution of the membrane voltage $V(t)$ of a passive neuron is described by the membrane equation \begin{equation} \label{passivemembrane} \tau \frac{dV}{dt} = -V + E \end{equation} where $\tau=10$\,ms is the membrane time constant and $E(t)$ is the reversal potential that also depends on time $t$. Such a differential equation can be numerically solved with the Euler method. For this the time is discretized by a time step $\Delta t=0.1$\,ms. The $i$-th time point is then at time $t_i = i \cdot \Delta t$. In matlab we get the time points $t_i$ simply by \begin{lstlisting} dt = 0.1; tmax = 100.0; time = [0.0:dt:tmax]; % t_i \end{lstlisting} When the membrane potential at time $t_0 = 0$ is $V_0$, the so called ``initial condition'', then we can iteratively compute the membrane potentials $V_i$ for successive time points $t_i$ according to \begin{equation} \label{euler} V_{i+1} = V_i + (-V_i + E_i) \frac{\Delta t}{\tau} \end{equation} \begin{parts} \part Write a function that computes the time course of the membrane potential of the passive membrane. The function gets as input arguments the initial condition $V_0$, the vector with the time course of $E(t)$, the value of the membrane time-constant $\tau$, and the time step $\Delta t$. \part In order to test your function set $V_0=1$\,mV and $E(t)=0$ and compute $V(t)$ for $t_{max}=50$\,ms. Plot $V(t)$ and compare it to the expected result of $V(t) = \exp(-t/\tau)$. Vary the time step $\Delta t$ by factors of 10 and discuss accuracy of numerical solutions. What is a good time step? Why is $V=0$ the resting potential of this neuron? \part Response of the passive membrane to a step input. Set $V_0=0$. Construct a vector for the input $E(t)$ such that $E(t)=0$ for $t\le 20$\,ms or $t\ge 70$\,ms, and $E(t)=10$\,mV for $20$\,ms $<t<70$\,ms. Plot $E(t)$ and the resulting $V(t)$ for $t_{max}=120$\,ms. \part Response to sine waves. As an input we now use $E(t)=\sin(2\pi f t)$. Compute the time course of the membrane potential in response to this input ($t_{max}=1$\,s). Vary the frequency $f$ between 1 and 100\,Hz. Be careful with the units within the sine function --- $ft$ must be unitless. What do you observe? \part Filter function of the passive neuron. Measure the amplitude of the voltage responses evoked by the sinusoidal inputs as the maximum of the last 900\,ms of the responses. Plot the amplitude of the response as a function of input frequency. This is the filter function of the passive neuron. How does the filter function depend on the membrane time constant? \part Leaky integrate-and-fire neuron. The passive neuron can be turned into a spiking neuron by introducing a fixed voltage threshold. Whenever the computed membrane potential of the passive neuron crosses the voltage threshold a spike is generated and the membrane voltage is set to the reset potential $V_R$ that we here set to zero. ``Generating a spike'' only means that we note down the time of the threshold crossing as a time where an action potential occurred. The waveform of the action potential is not modeled. Here we use a voltage threshold of 1\,mV. Write a function that implements this leaky integrate-and-fire neuron by expanding the function for the passive neuron appropriately. The function returns a vector of spike times. Illustrate how this model works by appropriate plot(s) and input(s) $E(t)$, e.g. constant inputs lower and higher than the voltage threshold. \part Show the response of the leaky integrate-and-fire neuron to a sine wave $E(t)=A\sin(2\pi ft)$ with $A=2$\,mV and frequency $f=10$, 20, and 30\,Hz. \part Compute the firing rate as a function of the frequency of the stimulating sine wave ($A=2$\,mV and frequencies between 5 and 30\,Hz). For a spike train with $n$ spikes at times $t_k$ ($k=1, 2, \ldots n$) the firing rate is \begin{equation} \label{firingrate} r = \frac{n-1}{t_n - t_1} \end{equation} What do you observe? Does the firing rate encode the frequency of the stimulus? Look at the spike trains in response to the sine waves to figure out what is going on. \end{parts} \end{questions} \end{document}