1938
DOI: 10.1007/bf01321920
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Herstellung und Eigenschaften weitwinkliger optischer Interferenzerscheinungen

Abstract: Es werden genaue Vorsehriften angegeben, wie die yore Verfasser im Jahre 1911 beschriebenen weitwinkligen Interferenzerscheinungen herzustellen sind und es werden einige diesbeztigliche neue Beobachtungen mitgeteilt. In ~berein-stimmung mit den damaligen Ergebnissen wird bewiesen, daiS die elementare Lichtemission in Kugelwellen sich fortpflanzt, deren s~mtliche Teile kohSrent sind und darfiber hinaus wird gezeigt, dal] diese Wellen auch beziiglich der Intensitiitsverteilung die Merkmale einer Dipolstrahlung b… Show more

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Cited by 14 publications
(2 citation statements)
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“…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%
“…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%
“…This affirmation puzzled me a carried out on a rotating platform (the Sagnac experiment) was discussed as "Theoretische Physik". In that book a certain interference experiment theoretical knowledge was to be derived from G. Joos's one volume When I was a graduate student at ETH, some 40 years ago, much of our ...5 OCR Output Ac A = 4 Aw sin ¢ = 0.236 (2) which is to be compared with the prediction (A = 5700 AE, ¢ = 41°46') A = 0.230 i 0.005…”
mentioning
confidence: 99%