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Tophat beam







 

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From Wikipedia, the free encyclopedia
 


This is an old revision of this page, as edited by Geoffrey.landis (talk | contribs)at17:11, 5 March 2024 (link to gaussian to tophat converter; mention of propagation diffraction, added citation to Flat-top beam). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.
(diff)  Previous revision | Latest revision (diff) | Newer revision  (diff)

Inoptics, a tophat (also Flat-top[1]ortop-hat) beam such as a laser beam or electron beam has a near-uniform fluence (energy density) within a circular disk. It is typically formed by refractive[2]ordiffractive optical elements from a Gaussian beam. Tophat beams are often used in industry, for example for laser drilling of holes in printed circuit boards. They are also used in very high power laser systems, which use chains of optical amplifiers to produce an intense beam. Tophat beams are named for their resemblance to the shape of a top hat.

Due to diffraction, a beam cannot maintain a sharp-edged tophat cross-section for more than a short length of propagation, and the edges of the distribution will become increasingly fuzzy as the beam propagates forward.

See also

External links

  1. ^ Rüdiger Paschotta, Flat-top Beams, DOI: https://doi.org/10.61835/6ku . Retrieved 5 March 2024.
  • ^ Nam-Hyong Kim and Alissa Wilczynski (March 31, 2021). How to design a Gaussian to Top Hat beam shaper. Retrieved 5 March 2024.

  • Retrieved from "https://en.wikipedia.org/w/index.php?title=Tophat_beam&oldid=1211995777"

    Category: 
    Laser science
     



    This page was last edited on 5 March 2024, at 17:11 (UTC).

    This version of the page has been revised. Besides normal editing, the reason for revision may have been that this version contains factual inaccuracies, vandalism, or material not compatible with the Creative Commons Attribution-ShareAlike License.



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