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Layered structures waves

From the three-layer mode equation, (15.3), the values cutoff and the penetration depth of the evanescent wave in the cover media, dv c, can be found for the three-layer structure as ... [Pg.402]

Surface acoustic wave (SAW)-type chemical sensors exploit the propagation loss of the acoustic waves along layered structures consisting of at least a substrate covered by the CIM. [Pg.87]

Figure 1. Schematic view of the one-dimensional layered structure. The vertical lines denote discontinuities of refractive index distribution. The monochromatic plane wave is incident in the y direction with the electric field amplitude The amplitudes of reflected and transmitted waves are ref and, respectively. Figure 1. Schematic view of the one-dimensional layered structure. The vertical lines denote discontinuities of refractive index distribution. The monochromatic plane wave is incident in the y direction with the electric field amplitude The amplitudes of reflected and transmitted waves are ref and, respectively.
Special conical lenses have been developed for Lamb wave imaging of layered structures because the waves are dispersive the frequency can be varied to tune the Lamb wave angle of the specimen to the angle for which the lens is designed (Atalar and Kbymen 1989). Such lenses could similarly be used for Sezawa wave imaging and measurement, and also for other dispersive waves. It may be that for layered structures measurements of V(f) at fixed defocus will become as prevalent as V(z) (Atalar et al. 1995). [Pg.218]

When light is incident from the ambient side in the positive x direction, there is no wave propagating in the negative x direction inside the substrate. This means that Em+1 = 0. For the whole layered structure, the resulting complex reflection and transmission coefficients can be expressed by using the matrix elements of the total system transfer matrix of (6.8) ... [Pg.254]

FIGURE 4.3. (a) Schematic structure of a microcavity LED with an Alq emitting layer. The top mirror is the electron-injecting contact and the bottom mirror is a three-period dielectric quarter-wave stack (QWS) with Si02(n = 1.5) and SixNy(n = 2.2). (b) Electroluminescence spectrum from a cavity LED compared with that from a noncavity LED. The noncavity LED possesses the same layer structure as shown in (a), but has no QWS. [Pg.108]

Interstellar dusts could have a layered structure, as proposed by Greenberg (1998), of an icy mantle covering an organic-silicate core. On the way from an interstellar molecular cloud to protosolar nebula, interstellar dust could be modified by any thermal events, e.g., nebula gas heated by shock waves on an accreting disk or the absorption of solar radiation. [Pg.16]

Two-Dimensional Network Containing an Undulated Wave Layer Structure... [Pg.277]

Well investigated stratified periodical structures (SPSs) are widely used as dielectric mirrors, polarization devices for integrated optics, tunable narrow band filters, time delay devices, nonreciprocal elements, devices of parametric and non-linear optics [1], The two-layer SPSs are a particular case of more general class of three-layer structures. For example, the three-layered structures (ABB) A with layers A and B and number of periods N can be considered as a two-layer SPS. In the paper we present features of optical wave transformation in three-layer periodical structures. [Pg.72]

Fendorf S, Wielinga BW, Hansel CM (2000) Chromium transformations in natural environments The role of biological and abiological processes in chromium(VI) reduction. Int Geol Rev 42 691-701 Fenter P, Cheng L, Rihs S, Machesky M, Bedzyk MJ, Sturchio NC (2000c) Electrical double-layer structure at the mtile-water interface as observed in situ with small-period X-ray standing waves. J Colloid Interface Sci 225 154-165... [Pg.81]

PROFILING THE ELECTRICAL DOUBLE LAYER STRUCTURE WITH X-RAY STANDING WAVES... [Pg.256]

The existence of an evanescent wave was discussed above (cf. Section III), together with PSPs. The optical properties of thicker LBK films can be characterized by the optical waveguide spectroscopy (WGS), and their layered structure can be probed by means of X-ray reflectometry. [Pg.138]

Different positions of the features in the spectra of samples with Mg2Si buried in Si matrix layers and of those with unburied ones lead us to the conclusion that two systems have to be considered (1) for the unburied layers, air/Mg2Si/Si (2) for buried layers air/Si/Mg2Si/Si. The dispersion relations are calculated from the boundary condition for a continuity of the polariton electric field by the method [2]. The calculations for three- and four-layered structures, obtained by Mills and Maradudin [2] and Nakayama et al. [6], respectively, were reproduced. We derived equations for polariton frequency co as a function of the polariton wave-vector k. Having into account that only when the condition k < caj (G>) I c... [Pg.212]


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See also in sourсe #XX -- [ Pg.207 ]




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