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Beam divergence

About: Beam divergence is a research topic. Over the lifetime, 5626 publications have been published within this topic receiving 73775 citations.


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Journal ArticleDOI

[...]

02 Aug 2002-Science
TL;DR: A periodic texture on the exit side of a single aperture in a metal film is created and, when combined with enhanced transmission, suggests that a wide range of photonic applications is possible.
Abstract: Light usually diffracts in all directions when it emerges from a subwavelength aperture, which puts a lower limit on the size of features that can be used in photonics. This limitation can be overcome by creating a periodic texture on the exit side of a single aperture in a metal film. The transmitted light emerges from the aperture as a beam with a small angular divergence (approximately ±3°) whose directionality can be controlled. This finding is especially surprising, considering that the radiating region is mainly confined to an area with lateral dimensions comparable to the wavelength of the light. The device occupies no more than one cubic micrometer and, when combined with enhanced transmission, suggests that a wide range of photonic applications is possible.

1,749 citations

Journal ArticleDOI

[...]

TL;DR: It is shown that, in the particular case of a tightly focused, radially polarized beam, the polarization shows large inhomogeneities in the focal region, while the azimuthally polarized beam is purely transverse even at very high numerical apertures.
Abstract: Cylindrical-vector beams are of increasing recent interest for their role in novel laser resonators and their applications to electron acceleration and scanning microscopy. In this paper, we calculate cylindrical-vector fields, near the focal region of an aplanatic lens, and briefly discuss some applications. We show that, in the particular case of a tightly focused, radially polarized beam, the polarization shows large inhomogeneities in the focal region, while the azimuthally polarized beam is purely transverse even at very high numerical apertures.

1,323 citations

Journal ArticleDOI

[...]

John U. White1
TL;DR: In this article, an absorption cell is described, in which the light traverses a small volume a large and arbitrarily variable number of times, and the angular aperture of the mirrors is not occulted either on or off the optical axis, and can be used for observing spectra that are very weak, or that belong to high boiling point compounds or to compounds obtainable only in very low concentrations.
Abstract: THE measurement of the vapor phase spectra T of compounds having high boiling points presents an experimental problem that may be solved either by heating the absorption cells or by making them very long. In the infra-red region radiation from the hot gases in heated cells decreases the accuracy of absorption measurements. If only a small amount of sample is available, the only possibility is to use an optical system in which the radiation goes back and forth through the same volume a large number of times. Several designs for such systems have been published recently1' 2 but none of them permits the use of large angular apertures at points off the optic axis. In this paper an absorption cell is described in which the light traverses a small volume a large and arbitrarily variable number of times, and in which the angular aperture of the mirrors is not occulted either on or off the optical axis. The design gives very high light transmission and can be used for observing spectra that are very weak, or that belong to high boiling point compounds or to compounds obtainable only in very low concentrations. It can be used for any liquids or gases that do not injure the mirror surfaces, with which they are directly in contact. The essential parts of the equipment are three spherical, concave mirrors that all have the same radius of curvature. These are set up as shown in Fig. 1 with two mirrors A and A' close together at one end of the absorption cell, and the third mirror B at the other end. The centers of curvature of A and A' are on the front surface of B, and the center of curvature of B is halfway between A and A'. This arrangement establishes a system of conjugate foci on the reflecting surfaces of the mirrors, by which all the light leaving any point on A is brought to a focus by B at the corresponding point on A', and all the light leaving this point on A' is focused back again to the

1,171 citations

Book ChapterDOI

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01 Jan 2007

584 citations

Journal ArticleDOI

[...]

TL;DR: In this article, it was shown that light impinging on isolated subwavelength holes in real metal film, in this case Ag, excite localized surface plasmon modes on the aperture ridge, which gives rise to optical tunneling with unexpected enhanced transmission peaks and directionality.
Abstract: A subwavelength aperture is a key element in near-field optical devices and many recent photonic structures When the lateral dimensions of such aperture is smaller than half the wavelength, light cannot propagate through the hole and the transmission is typically very weak It is usually believed to scale as the fourth power of the aperture diameter, a result first stated by Bethe [Phys Rev 66 (1944) 163] in 1944 by analyzing the transmission through a small hole in an infinitely thin perfectly metal screen However, a real subwavelength aperture is very different because the thickness and the finite conductivity of the metal has significant consequences which are far from being well understood Here we report that light impinging on isolated subwavelength holes in real metal film, in this case Ag, excite localized surface plasmon modes on the aperture ridge Their activation gives rise to optical tunneling with unexpected enhanced transmission peaks and directionality These properties follow from the dipolar nature of the LSP modes and can be tuned by an appropriate design of the aperture shape These findings are of relevance for the current trends in subwavelength optics

406 citations

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Performance
Metrics
No. of papers in the topic in previous years
YearPapers
202331
202281
202153
202086
201995
201884