Hexadecagon: Difference between revisions

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{{Unreferenced stub|auto=yes|date=December 2009}}
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The '''Charged current''' interaction is one of the ways in which subatomic particles can interact by means of the [[weak force]]. It is mediated by the [[W and Z bosons|{{SubatomicParticle|W boson+}} and {{SubatomicParticle|W boson-}} bosons]].
 
The interaction is often incorrectly believed to be called 'charged' because the W bosons have [[electric charge]]. However, the charged current that gives the interaction its name is that of the interacting particles. For example, the charged-current contribution to the {{SubatomicParticle|Electron neutrino}}{{SubatomicParticle|Electron}} → {{SubatomicParticle|Electron neutrino}}{{SubatomicParticle|Electron}} elastic scattering amplitude
 
<math>\mathfrak{M}^{\mathrm{CC}} \propto J_{\mu}^{\mathrm{(CC)}}(\mathrm{e^{-}}\to\nu_{\mathrm{e}}) \; J^{\mathrm{(CC)}\mu}(\nu_{\mathrm{e}}\to\mathrm{e^{-}})</math>
 
where the charged currents describing the flow of one [[fermion]] into the other are given by
 
<math>J^{\mathrm{(CC)\mu}}(f\to f') = \bar{u}_{f'}\gamma^{\mu}\frac{1}{2}\left(1-\gamma^{5}\right)u_{f}.</math>
 
==See also==
* [[Neutral current]]
 
{{DEFAULTSORT:Charged Current}}
[[Category:Electroweak theory]]
 
 
{{Particle-stub}}

Latest revision as of 23:30, 1 December 2014

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