“…Analytical equations for the shape of these caustics for an arbitrary location of the internal source were also derived by using the method employed in Appendix A of Ref. 15. Figure 7(d) shows a composite of the 1, 2, and 1 ϩ 2Ј interior caustics.…”
Section: Experimental Observation Of High-order Internal Cusp Causticsmentioning
confidence: 99%
“…11,12 But when a point source is brought close to the sphere, the p ϭ 1 near-zone spherical aberration caustic splits into two branches and evolves into a far-zone rainbow. 13 The interior caustics of a sphere include the so-called p ϭ 1 Descartes ring, which is the extension of the spherical aberration cusp into the sphere, 14 and various cusp caustics and axial spike caustics [15][16][17] for p у 2. The p ϭ 1 Descartes ring, enhanced by morphologydependent resonances, has been observed at the surface of both water and methanol droplets by means of stimulated Raman scattering (SRS).…”
Section: Introductionmentioning
confidence: 99%
“…2 The full p ϭ 2 axial spike caustic has also been observed in a spherical globe filled with water into which a small amount of milk had been added. 15 For scattering by an oblate spheroidal particle with side-on incidence, the rainbow evolves into a higherdimensional optical caustic whose full structure unfolds as the spheroid refractive index and eccentricity are varied. The unfolding of this caustic for p ϭ 2 has been numerically and analytically explored by Nye,22,23 and the unfolding as a function of spheroid eccentricity has been experimentally studied by Marston and his co-workers for p ϭ 2, 24-27 p ϭ 3, 28 and p ϭ 6.…”
“…Analytical equations for the shape of these caustics for an arbitrary location of the internal source were also derived by using the method employed in Appendix A of Ref. 15. Figure 7(d) shows a composite of the 1, 2, and 1 ϩ 2Ј interior caustics.…”
Section: Experimental Observation Of High-order Internal Cusp Causticsmentioning
confidence: 99%
“…11,12 But when a point source is brought close to the sphere, the p ϭ 1 near-zone spherical aberration caustic splits into two branches and evolves into a far-zone rainbow. 13 The interior caustics of a sphere include the so-called p ϭ 1 Descartes ring, which is the extension of the spherical aberration cusp into the sphere, 14 and various cusp caustics and axial spike caustics [15][16][17] for p у 2. The p ϭ 1 Descartes ring, enhanced by morphologydependent resonances, has been observed at the surface of both water and methanol droplets by means of stimulated Raman scattering (SRS).…”
Section: Introductionmentioning
confidence: 99%
“…2 The full p ϭ 2 axial spike caustic has also been observed in a spherical globe filled with water into which a small amount of milk had been added. 15 For scattering by an oblate spheroidal particle with side-on incidence, the rainbow evolves into a higherdimensional optical caustic whose full structure unfolds as the spheroid refractive index and eccentricity are varied. The unfolding of this caustic for p ϭ 2 has been numerically and analytically explored by Nye,22,23 and the unfolding as a function of spheroid eccentricity has been experimentally studied by Marston and his co-workers for p ϭ 2, 24-27 p ϭ 3, 28 and p ϭ 6.…”
“…For this θ i 0 interval, the horizontal radius of curvature R is now negative, corresponding to rays intersecting the exit plane in the horizontal direction as they converge toward an effective point source on the real caustic. There is also a virtual axial spike caustic [34] formed by the backprojection of the rays in all planes of incidence with the same deflection angle Θ 0 . These projections all cross the z axis at…”
The electromagnetic fields scattered when a plane wave is incident on an oblate spheroid in the side-on orientation may be calculated using a generalization of Mie theory, and the results may be decomposed in a Debye series expansion. A number of optical caustics are observed in the computed scattered intensity for the one internal reflection portion of the Debye series for scattering angles in the vicinity of the firstorder rainbow, and are analyzed in terms of the rainbow, transverse cusp, and hyperbolic umbilic caustics of catastrophe optics. The specific features of these three caustics are described, as is their assembly into the global structure of the observed caustics for spheroid scattering. It is found that, for a spheroid whose radius is an order of magnitude larger than the wavelength of the incident light, the interference structure accompanying the transverse cusp and hyperbolic umbilic caustics is only partially formed.
“…27 Thus it is of interest to inquire whether the p ϭ 1 scattering resonance/total internal reflection rainbow of Fig. 12(b) at Ϸ 135°remains visible in I total ave (r, , ).…”
Section: Semiclassical Scattering Of a Distribution Of Electric Dipolmentioning
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