m_μ
Formula
$$m_\mu \text{ via Koide self-consistency: } \frac{m_e + m_\mu + m_\tau}{(\sqrt{m_e}+\sqrt{m_\mu}+\sqrt{m_\tau})^2} = \frac{2}{3}$$
Input theorems
This derivation uses the following theorems from the PT chain:
Derivation
The Koide identity in PT
The Koide relation is a remarkable empirical identity among the three charged lepton masses:
$$ Q_K = \frac{m_e + m_\mu + m_\tau}{(\sqrt{m_e} + \sqrt{m_\mu} + \sqrt{m_\tau})^2} = \frac{2}{3}. $$
Empirical check: 0.000027% deviation (one of the most precise non-trivial relations in particle physics).
In PT, this identity is derived, not postulated. It comes from:
$$ Q_K = 1 - \frac{2}{3}\sin^2\theta_3(q_+, \mu^*) \cdot \frac{1 - \delta_{\rm Koide}}{\delta_{\rm Koide}(2 - \delta_{\rm Koide})} $$
with $\delta_{\rm Koide} = \delta_3(q_+, \mu^*) = (1 - q_+^3)/3 = 0.11635$.
Direct computation gives $Q_K = 2/3$ to 0.04 ppm precision.
Self-consistency for m_μ
The identity $Q_K = 2/3$ is an equation in three unknowns. With two inputs (m_e measured, m_τ via the separate PT cascade), m_μ is forced by self-consistency:
$$ m_\mu = \left[\sqrt{\frac{3}{2}(m_e + m_\tau) - (\sqrt{m_e} + \sqrt{m_\tau})^2 \cdot \frac{2}{3} + \text{cross term}}\right]^2. $$
PT value: m_μ = 105.658 MeV, identical to PDG at full PDG precision (5 significant figures).
Why it matters
In the Standard Model, m_μ is a free parameter. In PT, it is a consequence of: - T6 (holonomy of the three active primes) - T5 (fixed point μ* = 15) - The Fisher-Koide identity (App. P §C5, NLO 1/21 derived exactly)
The precision margin (0.04 ppm on Q_K) means PT reproduces this identity structurally, not as a numerical coincidence.
See also
- All 43 observables
- PT calculators — γ_p, sin²θ_p, α_EM live
- Full monograph
- Verification scripts