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Due to the comparatively thick barrier between the QW and QD, no electric coupling between QW and QD layers is expected [21].
The advantage of this design flow is its accurate mechanical simulation, but it lacks a method for analyzing the dynamic parasitic electrostatic effects arising from the electric coupling between (stationary) wiring and structures in motion.
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We expect galvanic coupling between the high conductive sedimentary basin and the deep conducting basement by the downward leakage of electric currents within the fault.
Strong electric coupling is achieved between adjacent resonators.
By running numerical integrations with increasing η, we observe the excitation activity to become spatiotemporally self-organized, until η is so strong that spoils sync between networks for a given value of the electric coupling strength.
Instead of using the ring reflector layer, the periodic stripes[13] and the periodic rings[14] have also been used to enhance the electric field coupling between the structures and nanoantennas which boost the electric fields at the gaps of nanoantennas.
F = qE for electric coupling, while F = T / L = μ B / L for magnetic coupling.
In this case, magnetic coupling holds important advantages over electric coupling.
For the magnetic coupling, T = μ B, while T = qEL in the case of the electric coupling.
Owing to asymmetric electric field coupling between the two resonators, the combined structure exhibits better performance in terms of transmission minima and bandwidths than the individual particles.
Also, finite element simulation of electric-solid coupling between displacement of piezoelectric diaphragm due to an applied voltage and resulting deformation of membrane was considered.
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