Several experiments search for μ↔e\documentclass[12pt]{minimal}
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\begin{document}$$\mu \leftrightarrow e$$\end{document} flavour change, for instance in μ→econversion\documentclass[12pt]{minimal}
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\begin{document}$$\mu \rightarrow e ~\mathrm{conversion}$$\end{document}, μ→eγ\documentclass[12pt]{minimal}
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\begin{document}$$\mu \rightarrow e \gamma $$\end{document} and μ→ee¯e\documentclass[12pt]{minimal}
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\begin{document}$$\mu \rightarrow e \bar{e} e$$\end{document}. This paper studies how to translate these experimental constraints from low energy to a New Physics scale M≫mW\documentclass[12pt]{minimal}
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\begin{document}$$M \gg m_W$$\end{document}. A basis of QCD ×\documentclass[12pt]{minimal}
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\begin{document}$$\times $$\end{document} QED-invariant operators (as appropriate below mW\documentclass[12pt]{minimal}
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\begin{document}$$m_W$$\end{document}) is reviewed, then run to mW\documentclass[12pt]{minimal}
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\begin{document}$$m_W$$\end{document} with one-loop Renormalisation Group Equations (RGEs) of QCD and QED. At mW\documentclass[12pt]{minimal}
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\begin{document}$$m_W$$\end{document}, these operators are matched onto SU(2)-invariant dimension-six operators, which can continue to run up with electroweak RGEs. As an example, the μ→eγ\documentclass[12pt]{minimal}
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\begin{document}$$\mu \rightarrow e \gamma $$\end{document} bound is translated to the scale M, where it constrains two sums of operators. The constraints differ from those obtained in previous EFT analyses of μ→eγ\documentclass[12pt]{minimal}
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\begin{document}$$\mu \rightarrow e \gamma $$\end{document}, but they reproduce the expected bounds on flavour-changing interactions of the Z and the Higgs, because the matching at mW\documentclass[12pt]{minimal}
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\begin{document}$$m_W$$\end{document} is pragmatically performed to the loop order required to get the “leading” contribution.
