← The BQ algebra at the Dirac level

BQ-Dirac Lorentz Transformations: Weyl and Dirac

The same boost along I, written in the two representations. In the Weyl representation the boost is ΛW = diag(U−1, U), the doubled Pauli rotor of the previous three models. The Dirac boost is not new: it is ΛW carried over by the Weyl-to-Dirac matrix S. Choose a four-vector and a velocity to see the boost of a in both representations side by side. The boosted coordinates come out the same in both; only the 4×4 matrices that hold them differ.

ΛW = e(ψ/2)σIW,   ΛD = e(ψ/2)σID = SΛWS−1,   aL = ΛaΛ−1 in both,   S = 1⁄√2[[1, 1], [−1, 1]]

Vector and boost

The two boost matrices

The exponential form: Λ = e(ψ/2)σI in both representations

The boost of a in both representations

From ΛW to ΛD through S

How the Dirac boost mixes time and space

What it means for spinors

Check by explicit 4×4 matrix multiplication

What changes and what does not

Changed by S: the matrices Λ, a, aL and the spinor Ψ. Not changed: the coordinates aμ and a′μ, the rotor form c𝟙 − sαI, the invariant aa = −(a0² − a²)𝟙, and the rotations diag(r, r), which are the same matrices in both representations. The boost is the one transformation whose matrix changes character: block diagonal in Weyl, inter-block in Dirac.

Sources and status

S and the Dirac basis follow de Haas (2026), From Weyl to Dirac, eqs. 1–24; ΛW = diag(U−1, U), ΨL = ΛΨ and ΛD2 follow de Haas (2025), BQ Dirac Gravity, eqs. 78–82 and 103–107. Reported, not changed: eq. 107 writes ΛD2 = 𝟙 cosh ψ + αI sinh ψ; with αID = [[0, −σI], [−σI, 0]] of From Weyl to Dirac eq. 14 the same matrix is cosh ψ 𝟙 − sinh ψ αID. The matrix [[cosh ψ 1, sinh ψ σI], [sinh ψ σI, cosh ψ 1]] itself agrees. The two agree if the αI of eq. 107 is the standard Dirac α = [[0, σI], [σI, 0]], which is σID = −αID on this page.

Every identity is checked exactly in bq_dirac_lorentz_representations.py. Part of the BQ algebra at the Dirac level; the Weyl-only boost is BQ-Dirac Lorentz transformations, the matrix S is on BQ Weyl and Dirac representations.