COMMENT This T-type calcium current was originally reported in Wang XJ et al 1991 This file supplies a version of this current identical to Quadroni and Knopfel 1994 except for gbar and Erev (see notes below). ENDCOMMENT NEURON { SUFFIX lva : NONSPECIFIC_CURRENT i USEION ca WRITE ica RANGE Erev,g, gbar, i RANGE k, alpha_1, alpha_2, beta_1, beta_2, V_s } UNITS { (S) = (siemens) (mV) = (millivolt) (mA) = (milliamp) } PARAMETER { gbar = 0.4e-3 (S/cm2) < 0, 1e9 > : Quadroni and Knopfel use 166e-6 Erev = 120 (mV) : orig from Wang XJ et al 1991 was 120 : note: Quadroni and Knopfel 1994 table 1 use 80 instead V_s = 0 (mV) : used to describe effect of changing extracellular [Ca] : 0 corresponds to [Ca]outside = 3 mM (p 841) } ASSIGNED { ica (mA/cm2) i (mA/cm2) v (mV) g (S/cm2) k alpha_1 (1) alpha_2 (1) beta_1 (1) beta_2 (1) } STATE { m h d } BREAKPOINT { SOLVE states METHOD cnexp g = gbar * m^3 * h ica = g * (v - Erev) i = ica : used only to display the value of the current (section.i_lva(0.5)) } INITIAL { LOCAL C, E : assume that v has been constant for a long time : (derivable from rate equations in DERIVATIVE block at equilibrium) rates(v) m = minf(v) : h and d are intertwined so more complex than above equilib state for m C = beta_1 / alpha_1 E = alpha_2 / beta_2 h = E / (E * C + E + C) d = 1 - (1 + C) * h } DERIVATIVE states{ rates(v) m' = (minf(v) - m)/taum(v) : alpham(v) * (1 - m) - betam(v) * m h' = alpha_1 * (1 - h - d) - beta_1 * h d' = beta_2 * (1 - h - d) - alpha_2 * d } FUNCTION minf(Vm (mV)) (1) { minf = 1.0 / (1.0 + exp(-(Vm + V_s + 63)/7.8)) } FUNCTION taum(Vm (mV)) (ms) { taum = (1.7 + exp( -(Vm + V_s + 28.8)/13.5 )) / (1.0 + exp( -(Vm + V_s + 63)/7.8) ) } PROCEDURE rates(Vm(mV)) { LOCAL tau_2 k = (0.25 + exp((Vm + V_s + 83.5)/6.3))^0.5 - 0.5 tau_2 = 240.0 / (1 + exp((Vm + V_s + 37.4)/30)) : same as tau2 p 842 equation (15) alpha_1 = exp( -(Vm + V_s +160.3)/17.8 ) : p 842 equation (14) beta_1 = k * alpha_1 alpha_2 = 1.0 / ( tau_2 * (1.0 + k) ) beta_2 = k * alpha_2 }