“…The character of the beam propagation behind the PhC depends on the wave front of the self-collimated beam. In particular, if the wave front of the beam acquires positive curvature (due to propagation in a material with negative or anomalous diffraction), then the beams can be focalized behind the modulated media [17]. The effect is related to superlensing (see [18] for theory and [19] for experiments in 2D PhCs, resulting in imaging of point sources by a PhC slice).…”
We experimentally observe formation of narrow laser beams behind the woodpile photonic crystal, when the beam remains well collimated in free propagation behind the crystal. We show that the collimation depends on the input laser beam's focusing conditions, and we interpret theoretically the observed effect by calculating the spatial dispersion of propagation eigenmodes and by numerical simulation of paraxial propagation model.
“…The character of the beam propagation behind the PhC depends on the wave front of the self-collimated beam. In particular, if the wave front of the beam acquires positive curvature (due to propagation in a material with negative or anomalous diffraction), then the beams can be focalized behind the modulated media [17]. The effect is related to superlensing (see [18] for theory and [19] for experiments in 2D PhCs, resulting in imaging of point sources by a PhC slice).…”
We experimentally observe formation of narrow laser beams behind the woodpile photonic crystal, when the beam remains well collimated in free propagation behind the crystal. We show that the collimation depends on the input laser beam's focusing conditions, and we interpret theoretically the observed effect by calculating the spatial dispersion of propagation eigenmodes and by numerical simulation of paraxial propagation model.
“…In addition to BG in the band structure (spectral dispersion relation), the periodic structure can also modify the spatial dispersion, allowing the managing of the diffractive broadening of beams [32,35,36]. The interaction of the spatial spectrum of the incident wave with the isofrequency curves of the modulated material can produce different focusing regimes depending on the curvature of the isolines in k-space, one example is the self-collimation discussed above.…”
Section: Angular Band Gapsmentioning
confidence: 99%
“…Due to that, one can observe different behaviour depending on the spatial dispersion relation, i.e., on the curvature of the isofrequency contours [32]. The socalled self-collimation effect, due to flat isofrequency contours, consists in the propagation of a beam in the periodic system without apparent diffraction keeping its original size.…”
“…The band gaps appear at high symmetry points in the Brillouin zone due to the presence of a degeneracy of the band structure produced by the Bragg interferences in the diffractive regime (λ a/2, λ being the wavelength of the incident wave and a the lattice constant characterizing the periodicity of the structure). Many interesting physical phenomena arise from this particular dispersion relation such as wave localization [2,3], excitation of evanescent waves [4,5], and relevant applications concerns filtering [6] and wave guiding [7][8][9]. In particular, many approaches have been proposed to degenerate the band and thus enlarge the band gaps [10][11][12].…”
Abstract:The acoustic properties of a three-dimensional sonic crystal made of square-rod rigid scatterers incorporating a periodic arrangement of quarter wavelength resonators are theoretically and experimentally reported in this work. The periodicity of the system produces Bragg band gaps that can be tuned in frequency by modifying the orientation of the square-rod scatterers with respect to the incident wave. In addition, the quarter wavelength resonators introduce resonant band gaps that can be tuned by coupling the neighbor resonators. Bragg and resonant band gaps can overlap allowing the wave propagation control inside the periodic resonant medium. In particular, we show theoretically and experimentally that this system can produce a broad frequency band gap exceeding two and a half octaves (from 590 Hz to 3220 Hz) with transmission lower than 3%. Finite element methods were used to calculate the dispersion relation of the locally resonant system. The visco-thermal losses were accounted for in the quarter wavelength resonators to simulate the wave propagation in the semi-infinite structures and to compare the numerical results with the experiments performed in an echo-free chamber. The simulations and the experimental results are in good agreement. This work motivates interesting applications of this system as acoustic audible filters.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.