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On the Koide-like Relations for the Running Masses of Charged Leptons, Neutrinos and Quarks
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Current experimental data indicate that the Koide relation for the pole masses of charged leptons, which can be parametrized as $Q^{pole}_l = 2/3$, is valid up to the accuracy of $O(10^{-5})$. We show that the running masses of charged leptons fail in satisfying the Koide relation (i.e., $Q_l(\mu) \neq 2/3$), but the discrepancy between $Q_l (\mu)$ and $Q^{pole}_l$ is only about 0.2% at $\mu=M_Z$. The Koide-like relations for the running masses of neutrinos ($1/3 < Q_\nu(M_Z) < 0.6$), up-type quarks ($Q_{U}(M_Z) \sim 0.89$) and down-type quarks ($Q_{D}(M_Z) \sim 0.74$) are also examined from $M_Z$ up to the typical seesaw scale $M_R \sim 10^{14}$ GeV, and they are found to be nearly stable against radiative corrections. The approximate stability of $Q_{U}(\mu)$ and $Q_{D}(\mu)$ is mainly attributed to the strong mass hierarchy of quarks, while that of $Q_l(\mu)$ and $Q_\nu(\mu)$ is essentially for the reason that the lepton mass ratios are rather insensitive to radiative corrections.
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Cited by 1 Pith paper
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A minimization theorem for the Koide ratio and its Standard Model calibration
Extending any positive-mass set by one particle minimizes the Koide ratio to Q0/(1+Q0) at m* = [(sum mi)/(sum sqrt(mi))]^2; adding the charm mass to leptons yields a value only 6 ppm above the ideal 2/5.
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