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4. Neurons in a network Fundamentals of Computational Neuroscience, T. P. Trappenberg, 2002. Lecture Notes on Brain and Computation Byoung-Tak Zhang Biointelligence Laboratory School of Computer Science and Engineering Graduate Programs in Cognitive Science, Brain Science and Bioinformatics Brain-Mind-Behavior Concentration Program Seoul National University E-mail: [email protected] This material is available online at http://bi.snu.ac.kr/ 1 Outline 4.1 Organizations of neural networks 4.2 Information transmission in networks 4.3 Population dynamics: modeling the average behavior of neurons 4.4 The sigma node 4.5 Networks with non-classical synapses: the sigma-pi node (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 2 4.1 Organizations of neural networks The high-order mental abilities An emerging property of specialized neural networks The number of neurons in the central nervous systems 1012 We aim to understand the principal organization of neuron-like elements and how such structures can support and enable particular mental processes. The anatomy of the brain areas Neocortex, cerebral cortex, cortex Cerebellum Subcortical area (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 3 4.1.1 Neocortical organization Brodmann’s cortical map 52 cortical area Functional correlates of different cortical areas Fig. 4.1 Outline of the lateral view of the human brain including the cortex, cerebellum, and brainstem. The neocortex is divided into for lobes. The numbers correspond to Brodmann’s classification of cortical areas. (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 4 4.1.2 Staining techniques Fig. 4.2 Examples of stained neocortical slice showing the layered structure in neocortex. (B) Illustration of different staining techniques. (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 5 4.1.3 Common neuronal types in the neocortex Pyramidal cell Stellate cell (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 6 4.1.4 The layered structure of neocortex A generally layered structure of the neocortex Laminar-specific structure Fig 4.2 A Fig 4.2 C Fig. 4.2 Examples of stained neocortical slice showing the layered structure in neocortex. (A) Nissl stained visual cortex showing cell bodies. (C) Different sizes of cortical layers in different areas. (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 7 4.1.5 Columnar organization and cortical modules Fig. 4.3 Columnar organization and topographic maps in neocortex. (A) Ocular dominance columns. (B) Schematic illustration of the relation between orientation and ocular dominance columns. (C) Topographic representation of the visual field in the primary visual cortex. (D) Topographic representation of touch-sensitive areas of the body I the somatosensory cortex. (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 8 (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 9 4.1.6 Connectivity between neocortical layers Fig. 4.4 Schematic connectivity patterns between neurons in a cortical layer. Open cell bodies represent (spiny) excitatory neurons such as the pyramidal neuron and the spiny stellate neuron. Their axons are plotted with solid lines that end at open triangles that represent the axon terminal. The dendritic boutons are indicated by open circles. Inhibitory (smooth) stellate neurons have solid cell bodies and synaptic terminal, and the axons are represented by dashed lines. (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 10 4.1.7 Cortical parameter (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 11 4.2 Information transmission in networks 4.2.1 The simple chain Biologically not reasonable A single presynaptic spike not sufficient to elicit a postsynaptic spike. Synaptic transmission is lossy. The death of a single neuron would disrupt the transmission. Fig. 4.5 (A) A sequential transmission line of four nodes. Parallel chains are made out of many such sequential transmission lies without connections between them. (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 12 4.2.2 Diverging-converging chains The number of neurons, N Divergence rate, m Convergence rate, C Fully connected network N=m=C Synaptic efficiency (weight), w Feedback loop Fig. 4.5 (B) Diverging/converging chains where each node can contact several other nodes in neighboring transmission chains. (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 13 4.2.3 Immunity of random networks to spontaneous background activity (1) Cortical neurons typically fire with some background activity Mean 5Hz, variance 3Hz Neuron that has 10000 excitatory dendritic synapses. Spiking arriving in each time interval (1ms) Mean μ = 10000 * 0.005 = 50 Variance σ2 = 0.003 A spike arriving at a synapse with weight w=1 would elicit a spike The neuron to be immune against the background firing. w < 1/50 = 0.02 (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 14 4.2.3 Immunity of random networks to spontaneous background activity (2) To compare these value to experimental data How to measure the average synaptic efficiency To stimulate a presynaptic neuron while recording from the postsynaptic neuron. Asynchronous gain The average number of extra spikes that are added to the spikes of a postsynaptic neuron by each presynaptic spikes. If 100 presynaptic spikes (100Hz) lead 2 postsynaptic spikes (2Hz) during 1ms, synaptic efficiency is 5/100 = 0.02 Fig. 4.6 Schematic illustration of the influence of a single presynaptic spike on the average firing rate of the postsynaptic neuron. The delay in the synaptic transmission curve is caused by some delay, after which, on average, more postsynaptic spikes are generated within a short time window compared to the spontaneous activity of the neurons (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 15 4.2.4 Noisy background Large variability Ex) μ = 50, variance σ2 = 50 The probability of a postsynaptic spikes generated by the background firing to be less than a certain value, pbg The probability of having more than x simultaneous presynaptic spikes ( y )2 dy 1 2 Gaussian distribution spikes 2 P( n x) e (4.1) If pbg = 0.1, x ≈ 59, 2 x w < 1/59 ≈ 0.017 1 x spikes P(n x) [1 erf ( )] 2 2 (4.2) x 2erf -1 (1 2 p bg ) (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr (4.3) 16 4.2.5 Information transmission in large random networks Previous condition, at least 59-50=9 additional presynaptic spikes to elicit a meaningful postsynaptic spike Large random networks 1010 Neurons Each of these neurons connects to 10000 other neurons Stimulate 1000 neurons 1000 * 10000 = 107 spikes transmitted The probability of a neuron receives A spike is 107 / 1010 Two spikes is (107 / 1010)2=10-6 Not sufficient to secondary spikes A consequence of the small number of connections per neuron relative to large number of neuron in the network (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 17 4.2.6 The spread of activity in small random networks Netlets Small networks with only a small number of highly efficient synapses. Only very few active presynaptic neurons can elicit a postsynaptic spike in functionally correlated neurons. Absolute Refractory Period Control the number of active neurons Two Asymptotic model Small initial activity we get an inactive netlet Initial large activity we get a nearly maximally active netlet (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 18 4.2.7 The expected number of active neurons in netlets The expected fraction of active nodes f f (t 1) (1 f (t ))(1 e f (t )C Fig. 4.7 The fraction of active nodes of netlets in the time interval t + 1 as a function of the fraction of active nodes in the previous time interval. The different curves correspond to different numbers of presynaptic spikes Θ that are necessary to elicit a postsynaptic spike. (A) Netlets with only excitatory neurons. (B) Netlets with the same amount of excitatory and inhibitory connections. 1 ( f (t )C ) n ) (4.4) n ! n 0 the average number of synapses per neuron, C the firing threshold, Θ attractive fixpoint, firing rate 500Hz 4.2.8 Netlets with inhibition Cortical neuron firing rate range 10~100Hz Inhibitory neurons the value still exceed. (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 19 4.3 Population dynamics: modeling the average behavior of neurons Simulation of networks of spiking neurons Computing power problem Use average firing rate Relationship of such models to population of spiking neurons What conditions these common approximations are useful and faithful descriptions of neuronal characteristics Rate models cannot incorporate all aspects of networks of spiking neurons Many investigations in computational neuroscience have used such models (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 20 4.3.1 Firing rate The rectangular time window The average temporal spike rate of a neuron with a window size Δt: v(t ) number of spike in ΔT 1 t ΔT / 2 (t 't f )dt ' ΔT Gaussian window v(t ) ΔT 1 2 t ΔT / 2 (t 't f )e(t 't ) (4.5) 2 / 2 2 dt ' (4.6) Fig. 4.8 (A) Temporal average of a single spike train with a time widow ΔT hat ahs to be large compared to the average interspike interval (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 21 4.3.2 Population averages The average population activity A(t) of neurons 1 number of spikes in population of size N T 0 T N 1 t T / 2 1 N lim (t 'tif )dt ' T 0 T t T / 2 N i 1 A(t ) lim Very small time windows A(t )dt 1 N (4.7) N (t 't i 1 f i ) (4.8) Fig. 4.8 (B) Pool or local population of neurons with similar response characteristics. The pool average is defined as the average firing rate over the neurons in the pool within a relatively small time window. (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 22 4.3.3 Population dynamics in response to slowly varying inputs The average behavior of a pool of neuron dA(t ) A(t ) g ( RI ext (t )) dt (4.9) Membrane time constant, τ Input current, I Activation function, g Stationary state dA 0 dt A(t ) g ( RI ext (t )) (4.10) (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 23 4.3.4 Rapid response of population Noise current at 100ms, increase external input current. Population dynamics(eqn 4.9) vs average population spike rate response to rapidly varying input. Adding noise, fluctuation, more realistic. Fig 4.9 (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr Fig. 4.9 Simulation of a population of 1000 independent integrate-and-fire neurons with a membrane time constant τm = 10 ms and threshold θ = 10. Each neuron receives an input with white noise around a mean RIext. this mean is switched from RIext = 11 to RIext = 16 at t = 100 ms. The spike count of the population almost instantaneously follows this jump in the input, whereas the average population rate, calculated from in eqn 4.9 with a linear activation function, follows this change input only slowly when the time constant is set to τ = τm . 24 4.3.5 Advanced descriptions of population dynamics ui (t ) (t t f ) wij (t t jf ) j t Spike response model t (4.11) Ignored ε term, i for the postsynaptic neurons, average 0 ij synaptic efficiency N (4.12) No spike-time adaptation in neuron. the mean influence of the postsynaptic potential f f j u (t ) 0 (t ' ) A(t t ' )dt ' 0 (4.13) Noise A(t ) Pu (t | t ) A(t )dt (4.14) g ( x) In slowly varying input, eqn 4.9 with a gain function, t t f f (4.15) f 1 ref log( 1 Fig. 4. 10 (A) The gain function of eqn 4.15 that can be used to approximate the dynamics of a population response to slowly varying inputs (adiabatic limit). (B) Examples of physiological gain functions from a hippocampal pyramidal cell. The discharge frequency is based on the inverse of the first interspike interval after the cell started to respond to rectangular current pulses with different strength (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 25 1 ) x 4.4 The sigma node McCulloch-Pitts node Rate model The timing of spikes is irrelevant. But spike times play critical role for fast response 4.4.1 Minimal neuron model Sigma node Rate value of neuronal groups, r Fig. 4.11 Schematic summary of the functionality of a sigma node most commonly used in networks of artificial neurons. Such a node weights the input value of each channel with the corresponding weight value of that channel and sums up all these weighted inputs. The output of the node is then a function of this internal activation. hi wi riin h hi i (4.16) (4.17) r out g (h) (4.18) r out g ( wi riin ) i (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 26 (4.19) 4.4.2 Common activation functions Activation function, g generalize the sigmoid function g (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr sig 1 1 exp( ( x x0 )) 27 (4.20) 4.4.3 The dynamic sigma node The discrete sigma node to continuous dynamics h(t t ) (1 t )h(t ) t r i i i (4.21) Continuous, limΔt→0. h(t t ) h(t ) dh(t ) h(t ) i ri h(t ) i ri (4.22) t dt i i Fig. 4.12 Time course of the activation of a leaky integrator node with initial value h = 0. In the lower curve no input Iin was applied leading to an exponential decay. The upper curve corresponds to a constant input current Iin = 0.5. The resting (4.23) activation of the node was set to hrest = 0.1. 4.4.4 Leaky integrator characteristics The leaky integrator dynamics. dh(t ) h(t ) r without external input dt i i i t Solve h(t ) h(0)e h rest (4.24) in i ri change behavior I i (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 28 4.4.5 Discrete formulation of continuous dynamics The exponential response to short inputs h(t t ) (1 e t t )h(t ) e r i i i (4.25) Taking time steps on a logarithmic scale Method Euler method Higher-order Runge-Kutta method Adaptive time step algorithm (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 29 4.5 Networks with non-classical synapses: the sigma-pi node Sigma node A very rough abstraction of real neuron Interaction of different ion channels Information-processing Nonlinear interaction between input channels Average firing rate 4.5.1 Logical AND and sigma-pi nodes Nonlinear interaction between two ion channels Firing threshold Requires at least two spikes in some temporal proximity Correspond to a logical AND function in in h w r Generalize this idea for model, sigma-pi node i jk j rk jk (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr (4.26) 30 4.5.2 Divisive inhibition Interaction between an excitatory synapse and an inhibitory synapse Divisive inhibition Shunting inhibition hi wik riexcitatory / rkinhibitory jk (4.27) (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 31 4.5.3 further sources of modulatory effects between synaptic inputs Fig. 4.13 Some sources of nonlinear (modulatory) effects between synapses as modeled by sigma-pi nodes. (A) shunting (divisive) inhibition, which is often recorded as the effect of inhibitory synapses on the cell body. (B) The effect of simultaneously activated voltage-gated excitatory synapses that are in close physical proximity to each other (synaptic clusters) can be larger than the sum of the effect of each individual synapse. Examples are clusters of AMPA ad NMDA type synapses. (C) some cortical synaptic terminals have nicotinic acetylcholine (ACh) receptors. An ACh releases of cholinergic afferents can thus produce a larger efflux of neurotransmitter and thereby increases EPSPs in the postsynaptic neuron of this synaptic terminal. (D) Metabotropic receptors can trigger intracellular messengers that can influence the gain of ion channels. (E) Ion channels can be linked to the underlying cytoskeleton with adapter proteins and can thus influence other ion channels through this link.0 (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 32 Conclusion The brain does display characteristic neuronal organizations Properties of networks of spiking neurons The spread of neuronal activities through random networks Transmission of information A sensible activity in random recurrent networks The self-organization of synaptic efficiencies The sigma node Modeling the average firing rate of populations of neurons Sigma-pi node Rate model (C) 2012 SNU CSE Biointelligence Lab, http://bi.snu.ac.kr 33