Universal Kernel

velocity space

The three-dimensional hyperbolic space of rest frames, on which the Lorentz group acts.

velocity spacethe sky: light directionsT⟨ξ, η⟩T = ξ†T−1ηgTg†=2111a step: own move or received exchangeform onto form: an isometry∞: ξ∞ = (1, 0)phase ω0: ξ0 = (0, 1)phase ωfuture-pointing: no past half, no shared sea
Plate W.26Records as points of velocity space, each carrying its form: a step of a history carries the record TT to gTg†gTg^\dagger and its form ξ†T−1η\xi^\dagger T^{-1}\eta onto the next record’s, and at the light directions the report states turn by phases.

As mathematics

H3=SL⁡(2,C)/SU(2)\mathbb H^3=\SL(2,\C)/\mathrm{SU}(2), the future unit timelike vectors of Minkowski space written as Hermitian 2×22\times2 matrices with SL⁡(2,C)\SL(2,\C) acting by X↦AXA†X\mapsto AXA^\dagger: equivalently the positive-definite Hermitian matrices of determinant one. Its sphere at infinity is P1(C)\Proj^1(\C), and [ψ]↦ψψ†[\psi]\mapsto\psi\psi^\dagger is an equivariant bijection from P1(C)\Proj^1(\C) onto the future null rays, under which rotations act as on the Bloch sphere and boosts by Möbius maps that are not isometries.

The Bianchi group PSL⁡(2,Z[ω])\PSL(2,\Z[\omega]) acts on it discretely with finite covolume, with cusps at the points of P1(Q(−3))\Proj^1(\Q(\sqrt{-3})), and the tessellation by regular ideal tetrahedra with one face at ∞\infty, 0, 1 has orientation-preserving symmetry group PGL⁡(2,Z[ω])\PGL(2,\Z[\omega]).

Its name in another fieldBridge
the positive-definite Hermitian 2×22\times2 matrices of determinant onebuilt
SL⁡(2,C)/SU(2)\SL(2,\C)/\mathrm{SU}(2), the future unit timelike vectorsclassical
the upper half-space, bounded by the celestial sphere P1(C)\Proj^1(\C)classical
the space of rest framesa reading
Builds
lift
In the dictionary
continuum