1965
DOI: 10.1103/physrev.138.b1561
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Electromagnetic Field in the Neighborhood of the Focus of a Coherent Beam

Abstract: An integral representation for the electromagnetic field in the region of focus of a coherent light beam that emerges from an aplanatic optical system has been derived by Ignatowsky (1919) and by Richards and Wolf (1959). In the present paper this representation is used to analyze the structure of the focal region in a typical case. Contours of the time-averaged electric energy density in the focal plane, in one defocused plane and in two meridional sections of the focal region of a system with angular semi-a… Show more

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Cited by 175 publications
(72 citation statements)
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“…Figures 3 and 4 clearly differ in appearance from their respective counterparts without refractive-index contrast. 7 If we move the lens closer to the interface, how much deeper will the point of maximum intensity then lie? This question is answered in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Figures 3 and 4 clearly differ in appearance from their respective counterparts without refractive-index contrast. 7 If we move the lens closer to the interface, how much deeper will the point of maximum intensity then lie? This question is answered in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…19,20 Note that, x and y correspond to the lateral axes and z is the optical axis. J 0 , J 1 and J 2 are Bessel functions of first kind.…”
mentioning
confidence: 99%
“…These state-of-art imaging systems are, widefield fluorescence microscopy, confocal microscopy and super-resolution 4pi microscopy. The system PSF h sys for a widefield microscope is, h(x, y, 28,29,27,30 In a confocal microscope, there is an additional pinhole P at the detector arm to eliminate out-of-focus light from the fluorescent sample. The system PSF for a confocal system can be expressed as h sys = h ill × (h det ⊗ P).…”
mentioning
confidence: 99%