The Maurer–Cartan Route to Isorapidity

The local rotor G = GφGr, fed by the rapidity fields, has its own canonical connection: the Maurer–Cartan form, projected on the flow, Ωτ = (DG/Dτ)G−1. Transported with the gravitational four-velocity Ug = G(cT̂)G† in the BQ triple product, its time channel is exactly the rate of the composed Lorentz factor:

[UgΩτ]T = (c/2) DΓ/Dτ,  Γ = cosh χr cosh χφ  — exact in the rapidities

Isorapidity, DΓ/Dτ = 0, is the statement that the connection has no boost rate along the flow. Step by step: a purely radial river cannot satisfy it, an azimuthal rapidity can, the Hubble river bounds the disk, and a virial closure at the bulge radius R fixes the constant and gives the rotation-curve law of the galaxy models. Choose the rapidities.

Rapidities feeding the rotor

Units: c = 1, rs = 2GM/c² = 1. Paper chart: χr = ψN − ψH = √(rs/r) − Hr/c, so vr = c tanh χr ≈ √(2GM/r) − Hr in slow flow. The galaxy-scale preset takes M ≈ 10¹¹ M⊙, R ≈ 2 kpc and a local Hz chosen so that rc ≈ 20R.

The rotation curve

From the rotor to the rotation curve in eight steps

BQ-Pauli level, following de Haas (2026), A Spin(1,3) Rapidity Theory for Galactic Rotation Curves, §2–3. Orthonormal spherical legs (Îr, Ĵθ, K̂φ) and (σ̂r, σ̂θ, σ̂φ) in the order (I, J, K). For a stationary, axisymmetric field D/Dτ = ur∂r with ur = c sinh χr.

The time channel along the flow

Check by explicit matrix multiplication

What this does and does not show

Rotor, Maurer–Cartan connection, triple product and the rotation law (eqs. 42–53) from de Haas (2026), A Spin(1,3) Rapidity Theory for Galactic Rotation Curves, and de Haas (2025), the SPARC fits of the Constant-Lagrangian model. Part of the BQ algebra models.