The local electronic structure characteristics in the contact region can non-trivially influence the conduction mechanism since, e.g., localized states do not contribute to the conduction, giving rise to conductance asymmetries and an overall loss of the transport information with respect to the ideal case.
In an anatomically detailed model of canine ventricular geometry, fiber architecture and Purkinje fiber network structure, a monodomain solution for anisotropic impulse conduction gave rise to electrical activation sequences that were consistent with experimentally observed patterns.
In theory, appropriately timed LV pacing can create fusion with intrinsic conduction, giving a similar effect as biventricular pacing.
Growth of the oxide film occurs by a succession of two high field ion conduction mechanisms given by i = Aexp (BV/x).
But the current in the gap region as a result of hopping conduction is given a little different.
The potential profile for the conduction electrons, given their lightness, is strongly modified by the effect of the laser field, whereas the deformation of the heavy-hole valence band is smaller.
The characteristic temperature dependence of hopping conduction is given by G T) = G0 exp[- T0/T 1/2] whexp[- T0/T 1/2efactor with T0 being a constant and originates from localized states induced by charge impurities [13–15].
The variation of ground temperature follows the one-dimensional, transient heat conduction equation given by Carslaw and Jaeger (1980): frac{{partial^{2} T y,t)}}{{partial y^{2} }} = frac{1}{alpha }frac{partial T y,t)}{partial t}.
One edge of the triangular quantum well is formed by a graded barrier; the other edge is formed by a fixed barrier as seen from the potential profile of the conduction band given in Figure 2. We have introduced the graded barrier in the structure in order to provide a quasi-electric field which facilitates the drift current of the photo-excited carriers to adjacent layers.
If volume conduction had given rise to systematic temporal variations of synchrony across conditions, the variations would be the same in the peak and opposite occipital areas in Experiment 1 because we see no reason to expect different volume conduction anisotropies in symmetrical cortical areas within the same temporal interval.
