Abstract:Surface acoustic waves (SAW’s) have been optically generated and detected on metallic spheres. The source was a focused yttrium aluminum garnet (YAG) laser operated in the Q-switched mode and the probe was a sensitive optical heterodyne interferometer. The curvature of the surface gives rise to dispersive effects. The variation of the SAW group velocity is deduced from the evolving waveforms of pulses detected after propagating a few turns around the sphere. The observation of SAW pulse waveforms at positions … Show more
“…The ratio of any two strengths among the longitudinal, shear, and Rayleigh waves depends on Poisson's ratio. It is known that the spherical Rayleigh wave is dispersive due to the surface curvature [9]. As seen in Fig.…”
Section: Experimental Measurementsmentioning
confidence: 67%
“…A similar study [9] reported measurements of Rayleigh waves generated on a sphere by a thermoelastic laser source and illustrated the general properties of this wave (e.g. the focusing at the poles and the wave dispersion).…”
Section: Experimental Measurementsmentioning
confidence: 92%
“…Instead of using direet integration to evaluate (5), eontour integration is more desirable and yields (9) where mn,i are the simple poles of E. As was shown in [13], the fundamental mode i=l and n>O forms the Rayleigh wave. For n=O, the sphere vibrates symmetrically with respeet to its center and hence these motions are denoted as the compressional modes.…”
“…The ratio of any two strengths among the longitudinal, shear, and Rayleigh waves depends on Poisson's ratio. It is known that the spherical Rayleigh wave is dispersive due to the surface curvature [9]. As seen in Fig.…”
Section: Experimental Measurementsmentioning
confidence: 67%
“…A similar study [9] reported measurements of Rayleigh waves generated on a sphere by a thermoelastic laser source and illustrated the general properties of this wave (e.g. the focusing at the poles and the wave dispersion).…”
Section: Experimental Measurementsmentioning
confidence: 92%
“…Instead of using direet integration to evaluate (5), eontour integration is more desirable and yields (9) where mn,i are the simple poles of E. As was shown in [13], the fundamental mode i=l and n>O forms the Rayleigh wave. For n=O, the sphere vibrates symmetrically with respeet to its center and hence these motions are denoted as the compressional modes.…”
“…A point-by-point study of laser-generated surface phonons on a sphere was carried out by Royer et al [2]. Because of the application to ball devices based on surface acoustic waves, there is much interest in characterizing how surface phonons propagate on the surfaces of elastically isotropic or anisotropic spheres [3].…”
Surface phonon wavepackets are generated on aluminium-coated transparent glass balls on irradiation with ultrashort light pulses. Delayed ultrashort probe light pulses are used to image the surface phonon propagation in real time by simply monitoring the modulation in the reflected probe beam intensity caused by the photoelastic effect. Imaging was achieved in the region of the phonon source and at the opposite pole of the sphere.
“…The profile of a circular wave front passing through a focus in 2D is known to undergo a shape change and a / 2 Gouy phase shift. 19,20 Our experimental resolution for ⌬ allowed us to study the former effect in detail but not the latter. The change in shape is governed by the complex value of the source function F 0 .…”
We use an ultrafast optical pump and probe technique to investigate the propagation of subgigahertz surface acoustic waves on a 1 mm diameter glass sphere with an aluminum coating. A fiber-based pump setup generates the surface waves and a common-path interferometer images them in the time domain over the sphere surface as they pass through the pole opposite the source of excitation. Fourier analysis allows the acoustic spectrum of the acoustic source to be extracted and waves traveling in opposite directions to be isolated.
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