The Projective Residue as a Schur Complement: Reduction of the Generation Split to the Chiral Asymmetry of Projection Locking

The fermionic sub-programme of Cosmochrony locates the three-generation mass split in the $J_3$-odd part of the squared projective endomorphism $E_\Pi^2$ restricted to the gauge-singlet generation triplet ${C^3_{\mathrm{gen}}}$, parametrised by a single real number $u$ through $E_\Pi^2|_{{C^3_{\mathrm{gen}}}}=\mathrm{diag}(1,\tfrac12+u,\tfrac12-u)$, with the even sector $\mathrm{diag}(1,\tfrac12,\tfrac12)$, the algebraic value of $(C_2-J_3^2)/C_2$ at $C_2=2$. Its reading as the Born–Infeld even sector would require an identification between the conditional $3\times3$ model of O30 on $\operatorname{Sym}^2(V_\rho)$ and $(E_\Pi^2)_{\mathrm{even}}$; no such identification is available, so that reading is not used here. This note fixes the structural status of $u$ before any explicit construction of $E_\Pi$. First, the projected Dirac square admits a universal Feshbach/Schur form $E_\Pi=-{\Pi_S}\,D\,(1-P)\,D\,{\Pi_S}^{*}=-M^{\dagger}M$ with $P={\Pi_S}^{*}{\Pi_S}$, exhibiting $E_\Pi$ as the Schur complement of the spinorial directions eliminated by the non-injective projection, negative semi-definite and vanishing in the injective limit. Second, the chiral block decomposition shows that $u$ is controlled by the ${\mathcal D}^{\pm}$-transported, generation-projected part of the antiunitary chiral equivariance defect \[ \Delta_\chi(P)=\pi_{LL}-\tau\,\overline{\pi_{RR}}\,\tau^{-1} \] of the eliminated block $1-P$, rather than by a naive block difference. Third, the minimal non-injectivity $c\leftrightarrow q-c$ is chirally symmetric, so $u=0$ at the level of axioms A1–A3; a non-zero $u$ requires a chiral symmetry-breaking carried by the projection-locking axiom A4. The finite locking sector is proved $J_\Pi$-equivariant, so $u_{\mathrm{fin}}=0$, and chirality is shown to be a Lorentzian rather than a finite-fibre datum. Finally, the Schur-transversality branch required by the Born–Infeld genus companion is closed in the present Lorentzian spin stratum: the projected A4 commutator has the exact metaplectic opening \[ \alpha(t,s)=ts\,\frac{r}{\sinh r}=ts+O\!\left((ts)^2\right),\qquad \mu(t,s)\equiv0, \] with $\cosh r=1+\tfrac{ts}{2}$, and its timelike Clifford symbol is not in the transported zero-mode locus. Together with the electric-genus result of the A4 companion, this promotes the existence statement to $u\neq0$ in the present stratum. The remaining open deliverables are the explicit Lorentzian eliminated block $1-P(s)$, the absolute normalisation $|u|$, and the projected Yukawa sector.

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-09-09
DOI
https://doi.org/10.5281/zenodo.22682251
Primary Topic
Black Holes and Theoretical Physics
Type
preprint
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The Projective Residue as a Schur Complement: Reduction of the Generation Split to the Chiral Asymmetry of Projection Locking

Jérôme Beau
Zenodo (CERN European Organization for Nuclear Research)
Black Holes and Theoretical Physics
preprint

The Projective Residue as a Schur Complement: Reduction of the Generation Split to the Chiral Asymmetry of Projection Locking

Jérôme Beau
preprint en

Abstract

The fermionic sub-programme of Cosmochrony locates the three-generation mass split in the $J_3$-odd part of the squared projective endomorphism $E_\Pi^2$ restricted to the gauge-singlet generation triplet ${C^3_{\mathrm{gen}}}$, parametrised by a single real number $u$ through $E_\Pi^2|_{{C^3_{\mathrm{gen}}}}=\mathrm{diag}(1,\tfrac12+u,\tfrac12-u)$, with the even sector $\mathrm{diag}(1,\tfrac12,\tfrac12)$, the algebraic value of $(C_2-J_3^2)/C_2$ at $C_2=2$. Its reading as the Born–Infeld even sector would require an identification between the conditional $3\times3$ model of O30 on $\operatorname{Sym}^2(V_\rho)$ and $(E_\Pi^2)_{\mathrm{even}}$; no such identification is available, so that reading is not used here. This note fixes the structural status of $u$ before any explicit construction of $E_\Pi$. First, the projected Dirac square admits a universal Feshbach/Schur form $E_\Pi=-{\Pi_S}\,D\,(1-P)\,D\,{\Pi_S}^{*}=-M^{\dagger}M$ with $P={\Pi_S}^{*}{\Pi_S}$, exhibiting $E_\Pi$ as the Schur complement of the spinorial directions eliminated by the non-injective projection, negative semi-definite and vanishing in the injective limit. Second, the chiral block decomposition shows that $u$ is controlled by the ${\mathcal D}^{\pm}$-transported, generation-projected part of the antiunitary chiral equivariance defect \[ \Delta_\chi(P)=\pi_{LL}-\tau\,\overline{\pi_{RR}}\,\tau^{-1} \] of the eliminated block $1-P$, rather than by a naive block difference. Third, the minimal non-injectivity $c\leftrightarrow q-c$ is chirally symmetric, so $u=0$ at the level of axioms A1–A3; a non-zero $u$ requires a chiral symmetry-breaking carried by the projection-locking axiom A4. The finite locking sector is proved $J_\Pi$-equivariant, so $u_{\mathrm{fin}}=0$, and chirality is shown to be a Lorentzian rather than a finite-fibre datum. Finally, the Schur-transversality branch required by the Born–Infeld genus companion is closed in the present Lorentzian spin stratum: the projected A4 commutator has the exact metaplectic opening \[ \alpha(t,s)=ts\,\frac{r}{\sinh r}=ts+O\!\left((ts)^2\right),\qquad \mu(t,s)\equiv0, \] with $\cosh r=1+\tfrac{ts}{2}$, and its timelike Clifford symbol is not in the transported zero-mode locus. Together with the electric-genus result of the A4 companion, this promotes the existence statement to $u\neq0$ in the present stratum. The remaining open deliverables are the explicit Lorentzian eliminated block $1-P(s)$, the absolute normalisation $|u|$, and the projected Yukawa sector.

Zenodo (CERN European Organization for Nuclear Research)
Black Holes and Theoretical Physics
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