2001
DOI: 10.1364/josaa.18.003085
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Semiclassical scattering of an electric dipole source inside a spherical particle

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Cited by 11 publications
(5 citation statements)
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References 31 publications
(45 reference statements)
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“…As shown, there is negligible ASE in the limit Im ǫ → 0, yet the localization of fluctuating dipoles to the gain-half of the (increasingly uniform) sphere leads to a small (though observable) amount of directionality, favoring emission toward the loss direction. The tendency of dipoles within a sphere to emit in a preferred direction has been studied in the context of fluorescence 94 in the ray-optical limit R ≫ c/ω, which as shown here is exacerbated in the presence of gain: 95 essentially, dipoles within a sphere tend to emit in the direction opposite the nearest surface, which explains why spheres having/lacking centro-symmetry tend to emit along directions of gain/loss. Moreover, in order to achieve large directivity, there needs to be a significant amount of mode confinement and gain, as illustrated by the negligible ASE and directivity of the Re ǫ = 2 sphere.…”
Section: Resultsmentioning
confidence: 91%
“…As shown, there is negligible ASE in the limit Im ǫ → 0, yet the localization of fluctuating dipoles to the gain-half of the (increasingly uniform) sphere leads to a small (though observable) amount of directionality, favoring emission toward the loss direction. The tendency of dipoles within a sphere to emit in a preferred direction has been studied in the context of fluorescence 94 in the ray-optical limit R ≫ c/ω, which as shown here is exacerbated in the presence of gain: 95 essentially, dipoles within a sphere tend to emit in the direction opposite the nearest surface, which explains why spheres having/lacking centro-symmetry tend to emit along directions of gain/loss. Moreover, in order to achieve large directivity, there needs to be a significant amount of mode confinement and gain, as illustrated by the negligible ASE and directivity of the Re ǫ = 2 sphere.…”
Section: Resultsmentioning
confidence: 91%
“…3,4 As r͞a approaches 1, the p ϭ 2 standard rainbow and the p ϭ 1 TIRR merge; this is because a point source located near the edge of the droplet will have the TIR region located almost directly behind it on the nearer edge of the droplet. 2 In principle, TIRRs can exist for all values of p, and the standard rainbow can exist for all p Ն 2, but we do not consider them in this paper, because they become faint; experimentally, we did not see any of the p Ͼ 2 rainbows. 3.…”
Section: Theorymentioning
confidence: 92%
“…2 In this paper we look only at what geometrical optics can tell us about this problem. Figure 1 shows a diagram of a droplet of radius a with a point source of light inside it at a distance r from the center.…”
Section: Theorymentioning
confidence: 99%
“…This study is indented to provide an in-depth analysis of the depolarization in the framework of Debye's series. The Debye series was first proposed by Debye for an infinite circular cylinder [12], and then has been extensively used for spherical particles [13][14][15][16], coated spherical particles [17][18][19][20][21][22][23], coated cylinder [24] and further extended to spheroidal particles based on the separation of the variable method [25][26]. The recent development of Debye's approach for non-spherical particles with the extended boundary condition method (EBCM) [27][28] is a breakthrough that makes it possible to perform accurate analyzes of the scattering mechanism by non-spherical particles.…”
Section: Introductionmentioning
confidence: 99%