TITLE K-A channel from Klee Ficker and Heinemann
: modified to account for Dax A Current ----------
: M.Migliore Jun 1997
: The original model results in too big window current, which is robably contamination of D-type current.
: To reduce the window current component, LSH changed vhalfn, zeatan and zetal as follows
: 1) vhalfn, 0 -> -15 mV
: 2) vhalfl, -60 -> -70 mV
: 3) zetan, -1.5 -> -3
: 4) zetal, 3 -> 5
: To fit these parameters to Kim Jonas (2012), they should be -5, -65, -1.8, 3.7, respectively.
UNITS {
(mA) = (milliamp)
(mV) = (millivolt)
}
PARAMETER {
v (mV)
celsius = 24 (degC)
gbar = .008 (mho/cm2)
vhalfn = -15 (mV)
vhalfl = -70 (mV)
a0l = 0.05 (/ms)
a0n = 0.05 (/ms)
zetan = -3 (1)
zetal = 5 (1)
gmn = 0.55 (1)
gml = 1 (1)
lmin = 6.7 (mS)
nmin = 0.1 (mS)
pw = -1 (1)
tq = -40
qq = 5
q10 = 5
qtl = 0.5
FRT = 39 (coulombs/joule)
}
NEURON {
SUFFIX KaProx
USEION k WRITE ik
RANGE gbar,gka,ik
GLOBAL ninf,linf,taul,taun,lmin
}
STATE {
n
l
}
ASSIGNED {
ik (mA/cm2)
ninf
linf
taul
taun
gka
}
INITIAL {
rates(v)
n=ninf
l=linf
}
BREAKPOINT {
SOLVE states METHOD cnexp
gka = gbar*n*l
ik = gka*(v+90.0)
}
FUNCTION alpn(v(mV)) {
LOCAL zeta
zeta = zetan + pw/(1+exp((v-tq)/qq))
alpn = exp(1.e-3*zeta*(v-vhalfn)*FRT)
}
FUNCTION betn(v(mV)) {
LOCAL zeta
zeta = zetan + pw/(1+exp((v-tq)/qq))
betn = exp(1.e-3*zeta*gmn*(v-vhalfn)*FRT)
}
FUNCTION alpl(v(mV)) {
alpl = exp(1.e-3*zetal*(v-vhalfl)*FRT)
}
FUNCTION betl(v(mV)) {
betl = exp(1.e-3*zetal*gml*(v-vhalfl)*FRT)
}
DERIVATIVE states { : exact when v held constant; integrates over dt step
rates(v)
n' = (ninf - n)/taun
l' = (linf - l)/taul
}
PROCEDURE rates(v (mV)) { :callable from hoc
LOCAL a,qt
qt=q10^((celsius-24)/10)
a = alpn(v)
ninf = 1/(a+1)
taun = betn(v)/(qt*a0n*(1+a))
if (taun<nmin) {taun=nmin}
a = alpl(v)
linf = 1/(a+1)
taul = 0.26*(v+50)/qtl
: taul = 0.26*v + 13.2, Hoffman Nat 98
if (taul<lmin/qtl) {taul=lmin/qtl}
}