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Revision as of 11:02, 15 July 2014 editRonnotel (talk | contribs)Extended confirmed users7,164 edits It works  Revision as of 17:36, 10 September 2014 edit undoRonnotel (talk | contribs)Extended confirmed users7,164 edits →Anomalous Dipole Moment: twitter versionNext edit →
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<math>\frac{g}{2}=1+\frac{\alpha}{2\pi}+\frac{2}{3}\alpha^2\left(\frac{\alpha}{2\pi}\right)-\frac{4}{3}\left(\frac{\alpha}{2\pi}\right)^2</math> <math>\frac{g}{2}=1+\frac{\alpha}{2\pi}+\frac{2}{3}\alpha^2\left(\frac{\alpha}{2\pi}\right)-\frac{4}{3}\left(\frac{\alpha}{2\pi}\right)^2</math>
<br>provides a value to the limit of experimental error. <br>provides a value to the limit of experimental error.

Twitter version:
g/2 = 1 + alpha/2pi + (2/3)*alpha^2*(alpha/2pi) - (4/3)*(alpha/2pi)^2

Revision as of 17:36, 10 September 2014

Anomalous Dipole Moment

Alternatively, the formula
g 2 = 1 + α 2 π + 2 3 α 2 ( α 2 π ) − 4 3 ( α 2 π ) 2 {\displaystyle {\frac {g}{2}}=1+{\frac {\alpha }{2\pi }}+{\frac {2}{3}}\alpha ^{2}\left({\frac {\alpha }{2\pi }}\right)-{\frac {4}{3}}\left({\frac {\alpha }{2\pi }}\right)^{2}}
provides a value to the limit of experimental error.

Twitter version: g/2 = 1 + alpha/2pi + (2/3)*alpha^2*(alpha/2pi) - (4/3)*(alpha/2pi)^2