Set
Then . Each involves only , so
for all . Their differentials have disjoint coordinate supports and are independent wherever none of them vanishes, which is an open dense regular set.
Hamilton's equations are
After the shift
they become independent harmonic oscillators,
Thus the independent commuting integrals establish complete integrability.
Completing the square gives
Hence the positive oscillator energy is
Using the convention
the integral is the phase-plane ellipse area divided by . With oscillator frequency , that area is . Therefore
Equivalently,
so the angle velocities are the constant frequencies .

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