The name is absent

61

per compartment and at most F gating variables per current, then we arrive at the
following system of ordinary differential equations

v^,(t) = Hv(t) — (Φ(w(i))e).v(i) + Φ(w(f))E_i + G(i).(v(t) - E_s), v(i) ∈ R^jv (3.2)

w'(i) = (Λ(v(t)) - »(t))./B(v(≠)), v(i) ∈ R^jv×^c×^f                            (3.3)

where H is the TV-by-# Hines matrix, e = [1 1 ∙ ∙ ■ l]^τ ∈ R^c,

Φ : R^λ,×^c×^f → R^7v ×^c_j G : R → R^7v,

A : R ^v → R^7v×^c×^f and B : R^jv → R^7v×^c×∙^f,

E_i is the vector of channel reversal potentials

ɛi = [Ecι E_Na Eχ ∙ ∙ ∙ ]^τ ∈ R^c,

E_s is the vector of synaptic reversal potentials

E_s = [E_ex E_ex E_in ∙ ■ ∙ ]^τ ∈ R^7v,

and the ‘dot’ operator, a.b, denotes element-wise multiplication and a.∕b denotes
elementwise division. In this section, we use only excitatory synapses with E_ex = 0

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