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.
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.
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.