Scale-relativistic corrections to the muon anomalous magnetic moment
The anomalous magnetic moment of the muon is one of the most precisely measured quantities in physics. Its experimental value exhibits a $4.2 \, σ$ discrepancy $δa_μ=(251 \pm 59) \times 10^{-11}$ with its theoretical value calculated in the standard model framework, while they agree for the electron. The muon theoretical calculation involves a mass-dependent contribution which comes from two-loop vacuum polarization insertions due to electron-positron pairs and depends on the electron to muon mass ratio $x=m_e/m_μ$. In standard quantum mechanics, mass ratios and inverse Compton length ratios are identical. This is no longer the case in the special scale-relativity framework, in which the Planck length-scale is invariant under dilations. Using the renormalization group approach, we differentiate between the origin of $ \ln x$ logarithmic contributions which depend on mass, and $x$ linear contributions which we assume to actually depend on inverse Compton lengths. By defining the muon constant $\mathbb{C}_μ=\ln(m_\mathbb{P}/m_μ)$ in terms of the Planck mass $m_\mathbb{P}$, the resulting scale-relativistic correction writes $δa_μ= -α^2 \, (x \:\ln^3 x)/(8 \; \mathbb{C}_μ^2)$, where $α$ is the fine structure constant. Its numerical value, $(230 \pm 16) \times 10^{-11}$, is in excellent agreement with the observed theory-experiment difference.