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Agreement of film shear moduli from both models, and of resonant film thickness from the parallel element equivalent circuit model and coulometric extrapolation of pre-resonant responses, supports the basic tenets of the film resonance model.
A simple example of the electromagnetic resonance model is the Ω-particle model, which describes the resonant induction for a conjugated bilayer gammadion structure [32].
If we combine the transverse resonance model with the reflection data from open ended quarter-wave resonators, we may improve convergence and reduce the computational error by a factor of 100.
We have presented a full wave transverse resonance model for a circular cylindrical annular geometry.
They become active in the presence of structural disorder as described by the double resonance model [37].
As a model problem we have used a full wave RF resonance model of [1] using transverse resonance method.
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This result is achieved by adjusting system parameters and thus obtaining a better matching of the input signals and resonance models.
No deviations from the Standard Model expectations are observed and stringent limits are set on the production cross-section times branching ratio of several resonance models.
The coefficients of normal forms related to different possible resonance models; namely, 1 2, 1 3, 1 4, 2 1, 3 1 and 4 1, are considered.
Finally, some simulation cases and experiments are conducted to verify the correctness of the harmonic resonance modeling, also the feasibility of proposed hybrid active power filter (HAPF) to attenuate the wideband-frequency harmonic currents is testified.
Even small variations in geometry can change decoding; for example, from the twenty nuclear magnetic resonance models of human ubiquitin in PDB 1C3T (CATH 3.10.20.90) the carbon backbones of the first and the second model align with RMSD (root mean square deviation) of 0.62 Å.
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