v \;=\; \underbrace{\color{#c0431d}m_\text{eff}\,c^2}_{\text{\footnotesize mass/energy}} \;\times\; \underbrace{\color{#1f5fa6}\sqrt{\nu}}_{\text{\footnotesize vacuum's condensation number}} \;\times\; \underbrace{\color{#a07820}\sqrt{8\pi}}_{\text{\footnotesize geometry}}
the Higgs vacuum expectation value v: the energy the vacuum carries in its ordered, symmetry-broken state, which gives the W, Z and every fermion its mass
m_\text{eff}\,c^2 \;=\; \frac{m_e\,c^2}{\alpha_{mf}} \;=\; \frac{0.511\ \text{MeV}}{0.3008} \;=\; 1.70\ \text{MeV}
\alpha_{mf} = \tan^2\theta_W, the measured Weinberg angle
\underbrace{0.51\ \text{MeV}}_{\substack{\text{visible: }30\%\\[1pt]\text{the electron's mass}}} \;+\; \underbrace{1.19\ \text{MeV}}_{\substack{\text{hidden: }70\%\\[1pt]\text{in counter-rotating seams}}} \;=\; 1.70\ \text{MeV}
\nu \;=\; \frac{m_\text{eff}}{m_1} \;=\; \frac{1.70\ \text{MeV}}{2.03\ \text{meV}} \;=\; 8.35\times10^{8}
m_1 c^2 = \hbar c/\xi, the vacuum particle at the 97 μm lattice cell
\sqrt{\nu} \;\approx\; 28{,}900
8\pi \;=\; \underbrace{2}_{\substack{\text{light-like}\\[1pt]\text{pressure}}} \times \underbrace{4\pi}_{\substack{\text{Gauss's law}\\[1pt]\text{(a sphere)}}}
the 4π of Newton’s \nabla^2\Phi = 4\pi G\rho; the 2 is \rho + 3P/c^2 = 2\rho for radiation
\sqrt{8\pi} \;=\; 5.01
v \;=\; {\color{#c0431d}1.70\ \text{MeV}} \times {\color{#1f5fa6}28{,}900} \times {\color{#a07820}5.01} \;=\; \boxed{246.1\ \text{GeV}} \qquad \text{measured: } 246.22\ \text{GeV}\quad(0.06\%)
no Higgs input and nothing fitted: the chain runs from the electron mass, the Weinberg angle and the dark-matter density, and never touches v