Reflection high-energy electron diffraction: Difference between revisions

Revision as of 12:51, 15 October 2021

Revision as of 06:53, 13 December 2021

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==Introduction==

A RHEED system requires an electron source (gun), photoluminescent detector screen and a sample with a clean surface, although modern RHEED systems have additional parts to optimize the technique.<ref name="ichimiya2004">{{cite book|author=Ichimiya A|author2=Cohen P I|name-list-style=amp|title=Reflection High Energy Electron Diffraction|publisher=Cambridge University Press: Cambridge, UK|date=2004|pages=1,13,16,98,130,161|url=https://books.google.com/books?id=AUVbPerNxTcC&printsec=frontcover|isbn=0-521-45373-9}}</ref><ref name="horio1996">{{cite journal|author=Horio Y|author2= Hashimoto Y|author3=Ichimaya A|name-list-style=amp|title=A new type of RHEED apparatus equipped with an energy filter| journal=Appl. Surf. Sci.|volume=100|pages=292–6|date=1996|doi=10.1016/0169-4332(96)00229-2|bibcode = 1996ApSS..100..292H }}</ref> The electron gun generates a beam of electrons which strike the sample at a very small angle relative to the sample surface. Incident electrons diffract from atoms at the surface of the sample, and a small fraction of the diffracted electrons interfere constructively at specific angles and form regular patterns on the detector. The electrons interfere according to the position of atoms on the sample surface, so the diffraction pattern at the detector is a function of the sample surface. Figure 1 shows the most basic setup of a RHEED system.

[[File:RHEED.svg|thumbnail|400px|'''Figure 1'''. Systematic setup of the electron gun, sample and detector /CCD components of a RHEED system. Electrons follow the path indicated by the arrow and approach the sample at angle θ. The sample surface diffracts electrons, and some of these diffracted electrons reach the detector and form the RHEED pattern. The reflected (specular) beam follows the path from the sample to the detector.]]

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===MCP-RHEED===

MCP-RHEED is a system in which an [[electron beam]] is amplified by a [[micro-channel plate]] (MCP). This system consists of an [[electron gun]] and an MCP equipped with a [[fluorescence|fluorescent]] screen opposite to the electron gun. Because of the amplification, the intensity of the electron beam can be decreased by several orders of magnitude and the damage to the samples is diminished. This method is used to observe the growth of [[Electrical insulation|insulator]] crystals such as [[Organic compound|organic]] films and [[alkali halide]] films, which are easily damaged by electron beams.<ref name="saiki">{{cite journal|author=Saiki K|author2=Kono T|author3=Ueno K|author4=Koma A|name-list-style=amp|title=Highly sensitive reflection high-energy electron diffraction measurement by use of micro-channel imaging plate|journal=Rev. Sci. Instrum.|volume=71|pages=3478|date=2000|doi=10.1063/1.1287625|bibcode = 2000RScI...71.3478S|issue=9 |s2cid=43346059|url=https://semanticscholar.org/paper/5d36f788118b97e81778e722e235469ca542cc63}}</ref>

==References==