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Compton scattering: Difference between revisions





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Xexno54 (talk | contribs)
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m →‎Introduction: Removed sentence fragment explaining (redundantly and in direct contradiction to the first sentence of the introduction) that Compton scattering is an example of elastic scattering, unused </ref> tag, and another strange, uncited sentence fragment about differing understandings of the elasticity of Compton scattering within different fields.
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[[File:Compton-en.svg|thumb|right|Fig. 1: Schematic diagram of Compton's experiment. Compton scattering occurs in the [[graphite]] target on the left. The slit passes X-ray photons scattered at a selected angle. The energy of a scattered photon is measured using [[Bragg scattering]] in the crystal on the right in conjunction with ionization chamber; the chamber could measure total energy deposited over time, not the energy of single scattered photons.]]
 
Compton scattering is an example of [[inelastic scattering]]. The incident photon loses energy in the lab frame, which centuries of practice had identified with inelastic scattering—even though, in the c.m. frame, the respective masses remaining the same, no new species are created and kinetic energy is conserved, the mark of an ''elastic collision''. As a result, HEP and nuclear physicists prefer to emphasize elasticity, while atomic and molecular physicists use "inelastic".</ref> of light by a free charged particle, where the wavelength of the scattered light is different from that of the incident radiation. In Compton's original experiment (see Fig. 1), the energy of the X ray photon (≈17 keV) was significantly larger than the binding energy of the atomic electron, so the electrons could be treated as being free after scattering. The amount by which the light's wavelength changes is called the '''Compton shift'''. Although nucleus Compton scattering exists,<ref>{{cite journal|title=Nuclear Compton scattering|author=P. Christillin|year=1986|journal= J. Phys. G: Nucl. Phys.|volume=12|pages=837–851|url=https://iopscience.iop.org/article/10.1088/0305-4616/12/9/008/meta|doi=10.1088/0305-4616/12/9/008|bibcode = 1986JPhG...12..837C|issue=9 |s2cid=250783416 }}</ref> Compton scattering usually refers to the interaction involving only the electrons of an atom. The Compton effect was observed by [[Arthur Holly Compton]] in 1923 at [[Washington University in St. Louis]] and further verified by his graduate student [[Wu Youxun|Y. H. Woo]] in the years following. Compton earned the 1927 [[Nobel Prize in Physics]] for the discovery.
 
The effect is significant because it demonstrates that light cannot be explained purely as a [[wave]] phenomenon.<ref>{{cite book

Retrieved from "https://en.wikipedia.org/wiki/Compton_scattering"
 




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