We discuss the relationship between response functions for systems having discrete resonances, as compared with those having branch-cut spectra, and highlight some of the advantages the latter may have in applications such as energy harvesting and design of metamaterials.
The all-important factor is the rise of new vibration branches of optical spectrum, namely, the interface optical phonon [1].
In each case, frequency spectra and physical through the thickness depictions of selected individual elastodynamic modes representative of the various branches of the spectrum are computed and compared.
Each of the three branches of the frequency spectrum for the Mindlin plate is associated with its corresponding branch of the frequency spectrum of the infinite elastodynamic plate through direct comparison.
Due to centrifugal distortion, a single pump and Stokes laser pulses cannot resonantly excite all the different rotational lines of any branch of the Raman spectra.
Our nonlinearity may cross multiple consecutive branches of the Fučík spectrum curves, and recent results in the literature are complemented and generalized.
The effect of the shear correction coefficient on the branches of the frequency spectrum for the free vibrations of Mindlin plates is studied.
Indeed the number, placement and properties of the inertial resonators can be designed to open, shift and enlarge the band gaps between one or more pairs of consecutive branches in the frequency spectrum.
where β = (p,μ) and the parameter μ = ± 1 labels two branches of the spin-split spectrum.
In this paper, we develop a theory of polarons in the quantum wires, taking into account the interaction of charged particles with all branches of the optical phonon spectrum.
Since the second-branch C 2 d of (1) is the first nontrivial branch of the simplest discrete Fučík spectrum, we believe that its properties can help to explain difficulties with discrete Fučík spectra.
