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Table I

Fitted Values for the Simulated Currents

α1Cβ2a
Forward voltage- independent coefficientBackward voltage-independent coefficient
ms−1  ms−1 
α01    0.0016  β01   0.0001 
α02   24.6178  β02  42.5775 
α03    0.0001  β03   0.0001 
α04  214.2350  β04   0.0001 
  [Ca2+    
α12    0.7958  β12   5.9780 
α13    0.0910  β13   1.4961 
α22    1.0000  β22   1.0000 
α23    0.1984  β23   0.1019 
α24    1.1180 [Ca2+ β24   0.0001 
αbk    1.0000  βbk   0.00727 
αb  161.7120  βb   0.67953 
αn    3.3940  βn   0.00135 
Charge (e Fraction of the field 
z1    0.2574  δ1   0.8246 
z2    0.0001  δ2   0.0001 
z3    2.9835  δ3   0.4307 
α1Cβ2a
Forward voltage- independent coefficientBackward voltage-independent coefficient
ms−1  ms−1 
α01    0.0016  β01   0.0001 
α02   24.6178  β02  42.5775 
α03    0.0001  β03   0.0001 
α04  214.2350  β04   0.0001 
  [Ca2+    
α12    0.7958  β12   5.9780 
α13    0.0910  β13   1.4961 
α22    1.0000  β22   1.0000 
α23    0.1984  β23   0.1019 
α24    1.1180 [Ca2+ β24   0.0001 
αbk    1.0000  βbk   0.00727 
αb  161.7120  βb   0.67953 
αn    3.3940  βn   0.00135 
Charge (e Fraction of the field 
z1    0.2574  δ1   0.8246 
z2    0.0001  δ2   0.0001 
z3    2.9835  δ3   0.4307 

Values of rates, charge, and fraction of the field in each transition for the model illustrated in Fig. 10. The rates are:

\begin{equation*}{\alpha}_{ij}(V)={\alpha}_{ij}e^{z_{j}{\delta}_{j}\frac{eV}{kT}}\end{equation*}
,
\begin{equation*}{\beta}_{ij}(V)={\beta}_{ij}e^{-z_{j}(1-{\delta}_{j})\frac{eV}{kT}}\end{equation*}
.  

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