Skip to content
DraconiticResearch
Search Sources API
203,234 studies31 sourcesUpdated 8 min ago
PreprintarXiv licencearXiv

The Doublet Tower of Cl(4,2): Universal Nilpotency, Projector Identities, and the sl(8,R) Parabolic from Conformal Null Vectors

Abstract

The conformal geometric algebra Cl(4,2) ~ R(8) carries a natural Z_2-grading defined by the dilatation bivector D=\e_4e_0, which satisfies D2=1 and splits the eight-dimensional spinor module into two four-dimensional eigenspaces S=S+⊕ S-. We prove that the ad_D-eigenvectors of Cl(4,2), those elements with eigenvalue~±1 under the Lie bracket [D,·], are exhausted by 16 doublets of the form T±J=n• eJ, where n• ∈ n∞,no is a null vector and eJ is a product of Lorentz-sector basis vectors indexed by J⊆{1,2,3,5}. These doublets satisfy universal algebraic identities: (T±J)2=0 (nilpotency) and T+J T-J=(−1)k(k+1)/2+1 ηJ 2Π+ (single-projector proportionality), where k=|J|, ηJ=∏j∈ Jηjj is the spectator metric, and Π+=1/2(1+D). The contracted sums ∑|J|=kT+J T-J are shown to be controlled by the elementary symmetric polynomials Sk of the Lorentz signature values (+1,+1,+1,−1), with the vanishing of S2=0 reflecting the (3,1) signature of physical spacetime. The even-grade doublets (belonging to Cl^+(4,2) ~ Cl(4,1)) contribute 8Π+ to the unweighted grand total, while the odd-grade doublets cancel exactly. The 32 doublet eigenvectors generate, under the commutator bracket, the 63-dimensional Lie algebra sl(8,R) in which the conformal algebra so(4,2) embeds as a 15-dimensional subalgebra. All identities, including a closed form for the commutators across the Levi interface, are proved in every conformal extension Cl(p+1,q+1); there the commutator span misses precisely the center of the algebra, a parity dichotomy invisible at the Lorentz signature. Two applications are developed: the top rung of the tower computes the Dirac versus Majorana dichotomy of rank-five pseudoscalars ... [shortened]

Related

  1. Siegel-Weil type identities for general linear groups related to parabolic induction from two Speh representations
    David Ginzburg, David Soudry
    arXivPreprintCC BY 4.0Full textAlgebra & number theoryarXiv
  2. Universal Cumulants and Conformal Invariance in Annihilating Random Walks with Pair Deposition
    D. Karevski, G M Schütz, A. Zahra
    Mathematical Physics, Analysis and GeometryPeer-reviewedCC BY 4.0Full textMathematical physicsCondensed matterHAL
  3. Universal Suppression of Dissipation across Conformal Interface in Open Quantum Critical Systems
    Ruhanshi Barad, Tian Wu, Qicheng Tang +1
    arXivPreprintarXiv licenceFull textMathematical physicsHigh-energy & particle physicsarXiv
  4. Homotopical Nilpotency and Homology Nilpotency: A Dimension--Connectivity Bound
    Paul-Eugene Parent
    arXivPreprintCC BY-NC-ND 4.0Full textGeometry & topologyarXiv
  5. On nilpotency in pre - Lie algebras
    Leonid Kurdachenko, Igor Subbotin
    arXivPreprintCC BY 4.0Full textAlgebra & number theoryarXiv
BibTeX
@misc{hansen2026doublet,
  title = {{The Doublet Tower of Cl(4,2): Universal Nilpotency, Projector Identities, and the sl(8,R) Parabolic from Conformal Null Vectors}},
  author = {Steen H. Hansen},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.22275},
  eprint = {2609.22275},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.22275},
}
RIS
TY  - UNPB
TI  - The Doublet Tower of Cl(4,2): Universal Nilpotency, Projector Identities, and the sl(8,R) Parabolic from Conformal Null Vectors
AU  - Steen H. Hansen
PY  - 2026
DA  - 2026/09/11
PB  - arXiv
DO  - 10.48550/arxiv.2609.22275
UR  - https://arxiv.org/abs/2609.22275
AB  - The conformal geometric algebra Cl(4,2) ~ R(8) carries a natural Z_2-grading defined by the dilatation bivector D=\e_4e_0, which satisfies D^2=1 and splits the eight-dimensional spinor module into two four-dimensional eigenspaces S=S_+⊕ S_-. We prove that the ad_D-eigenvectors of Cl(4,2), those elements with eigenvalue~±1 under the Lie bracket [D,·], are exhausted by 16 doublets of the form T^±_J=n_• e_J, where n_• ∈ n_∞,n_o is a null vector and e_J is a product of Lorentz-sector basis vectors indexed by J⊆{1,2,3,5}. These doublets satisfy universal algebraic identities: (T^±_J)^2=0 (nilpotency) and T^+_J T^-_J=(−1)^k(k+1)/2+1 η_J 2Π_+ (single-projector proportionality), where k=|J|, η_J=∏_j∈ Jη_jj is the spectator metric, and Π_+=1/2(1+D). The contracted sums ∑_|J|=kT^+_J T^-_J are shown to be controlled by the elementary symmetric polynomials S_k of the Lorentz signature values (+1,+1,+1,−1), with the vanishing of S_2=0 reflecting the (3,1) signature of physical spacetime. The even-grade doublets (belonging to Cl^+(4,2) ~ Cl(4,1)) contribute 8Π_+ to the unweighted grand total, while the odd-grade doublets cancel exactly. The 32 doublet eigenvectors generate, under the commutator bracket, the 63-dimensional Lie algebra sl(8,R) in which the conformal algebra so(4,2) embeds as a 15-dimensional subalgebra. All identities, including a closed form for the commutators across the Levi interface, are proved in every conformal extension Cl(p+1,q+1); there the commutator span misses precisely the center of the algebra, a parity dichotomy invisible at the Lorentz signature. Two applications are developed: the top rung of the tower computes the Dirac versus Majorana dichotomy of rank-five pseudoscalars ... [shortened]
ER  -