Namely, cross-sectional displacement and strain fields are composed of independent and orthogonal modes, which results in unambiguously defined generalised cross-sectional stress-resultants and in a minimisation of the coupling of equilibrium equations.
Note that, one way of performing prediction mode decision would exhaustively search the possibilities within a set containing all possible modes, which results in an undesirable complexity.
When the wavevector is perturbed, resonances occur around the trapped modes which results in transmission anomalies and dramatic field amplification in graphene stacks.
It is shown that these motions may give raise to bouncing modes, which results in high bearing forces and hence can be a possible cause of failure.
The near-field plasmon hybridizations between individual Ag nanodisks and the Ag substrate form four independent magnetic dipole modes, which result into multiband absorption enhancement of monolayer graphene in the visible wavelength range.
The near-field plasmon hybridizations between individual Ag nanodisks and the Ag substrate form four independent magnetic dipole modes, which result into multiband absorption enhancement of monolayer graphene at optical frequencies.
The near-field plasmon hybridizations between individual Ag nanodisks and the Ag substrate form four independent magnetic dipole modes, which result into four-band absorption enhancement of monolayer graphene.
In our designed metamaterials, the near-field plasmon hybridizations between individual Ag nanodisks and the Ag substrate form four independent magnetic dipole modes, which result into multiband absorption enhancement of monolayer graphene in the visible wavelength range from 450 to 800 nm, with an average absorption efficiency exceeding 50% (please see Fig. 2).
Despite the foregoing discussion on cell-to-cell variability, the inherent robustness in metabolic networks drive the physiological state to very few distinct modes, which results in multimodal distribution in response space.
The high-frequency Raman peak at 1,006 cm−1 corresponds to the vanadyl mode terminal oxygen stretching mode, which results from an unshared oxygen[23].
