1911
DOI: 10.1002/andp.19113400803
|View full text |Cite
|
Sign up to set email alerts
|

Über Lichtzerstreuung im Raume Wienerscher Interferenzen und neue, diesen reziproke Interferenzerscheinungen

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
4
0

Year Published

1924
1924
2020
2020

Publication Types

Select...
7
1

Relationship

0
8

Authors

Journals

citations
Cited by 27 publications
(4 citation statements)
references
References 2 publications
0
4
0
Order By: Relevance
“…We identify the interference fringes in Fig. 2 as in-plane scattering distributions of Selényi rings [9]. These rings are known to be centered around the mean surface normal, with their angular position being independent of the angle of incidence.…”
Section: Single Rough Interfacementioning
confidence: 99%
See 1 more Smart Citation
“…We identify the interference fringes in Fig. 2 as in-plane scattering distributions of Selényi rings [9]. These rings are known to be centered around the mean surface normal, with their angular position being independent of the angle of incidence.…”
Section: Single Rough Interfacementioning
confidence: 99%
“…For films with a thickness on the order of several wavelengths they were able to explain the periodic fringes they observed in the mean differential reflection coefficient through simple phase arguments. The patterns in the diffusely scattered light were shown to undergo a transition, with increasing surface roughness, from an intensity pattern exhibiting fringes whose angular positions are independent of the angle of incidence (Selényi rings [9]) to one with fringes whose angular positions depend on the angle of incidence (Quételet rings [7]) and eventually into a fringeless pattern with a backscattering peak, which is a signature of multiple scattering [10]. Although the Selényi rings are centered around the mean surface normal, with their position being independent of the angle of incidence, their amplitude, however, is modulated by the angle of incidence.…”
Section: Introductionmentioning
confidence: 99%
“…We observe that the diffuse component of the MDRC for the correlated systems oscillates weakly around that of the uncorrelated system. The physical origin of these oscillations is similar to that of the Selényi rings occurring in rough dielectric films [29,32,33]. The reason for the less pronounced effect is that only a thin layer, of thickness ε⊥ , contributes to the average interference effect, on top of the background signal coming from the thick layer of thickness L − ε⊥ whose dielectric fluctuations are not correlated to the surface.…”
Section: B Genuine Volume Configurationmentioning
confidence: 54%
“…Using the spacing between peaks in the moiré pattern, equal to L /2 n , we measured a spatial period of 4690 nm, accurate to within 3.8% of the theoretical value. Previous work has shown that when fluorescent molecules are placed close to a mirror, the emitting molecule acts as an oscillating dipole (an antenna) and that the reflected and unreflected parts of the emitted fluorescence wave interfere with each other, producing fringes from wide-angle interference 19 20 21 and oscillations in the fluorescence decay time 22 23 24 25 , with analytic expressions for the radiation patterns derived from electrodynamic theory 26 27 28 and modified further from the fixed-dipole amplitude assumption to model the fluorophore as a dipole of constant power and variable amplitude 29 30 . Subsequent work in this area studied the modulation of fluorescence intensity with distance from the mirror, and explained the modulation as a consequence of the interference effects of the excitation and of the emission being both present 31 .…”
Section: Resultsmentioning
confidence: 99%