Flavor-Singlet Tetrad Condensation and Monometric Emergent Geometry: A Large-N Functional-RG Framework
- 1Independent Researcher, Lima, Peru
Abstract
We investigate whether a multiflavor fermionic pregeometric framework can dynamically
select a single composite tetradic condensate from competing flavor channels. Within a
leading projected ladder/large-N functional-renormalization-group truncation, we analyze a
J = 2 channel whose dimensionless coupling obeys βg = 4g − ATg2, with AT > 0 under
the physical transverse-traceless susceptibility prescription adopted in the truncation. The
corresponding critical separatrix is g∗ = 4/AT. A flavor-dependent splitting permits the win
dow gS > g∗ >gA, so that the flavor singlet reaches the collective instability while a positive
subcritical adjoint branch remains below criticality. In the bosonized branch considered here,
singlet criticality is compatible with a nonzero tetradic condensate while the flavor-adjoint
directions retain positive quadratic curvature, yielding an operationally monometric phase
within the truncation. For a Hermitian physical transverse-traceless spin-2 channel with
nonzero spectral support and a well-defined subtracted dispersive representation, Källén
Lehmann positivity implies Zdisp
TT > 0. This result fixes only the dispersive contribution;
it does not determine local matching terms, the complete renormalized Planck coefficient,
or the full pole structure of the theory. The construction therefore provides a conditional
dynamical mechanism for selecting a single tetradic background from a multiflavor fermionic
system rather than a derivation of complete general relativity. Full Ward identities, local
matching, torsional dynamics, ghost tests outside the TT sector, and nonlinear completion
remain open problems for subsequent stages of the B-MECG research program
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BibTeX
@misc{barrantes2026flavorsinglet,
title = {{Flavor-Singlet Tetrad Condensation and Monometric Emergent Geometry: A Large-N Functional-RG Framework}},
author = {Victor Barrantes},
howpublished = {Zenodo},
year = {2026},
month = oct,
doi = {10.5281/zenodo.23556292},
url = {https://zenodo.org/records/23556292},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Flavor-Singlet Tetrad Condensation and Monometric Emergent Geometry: A Large-N Functional-RG Framework
AU - Victor Barrantes
PY - 2026
DA - 2026/10/22
PB - Zenodo
DO - 10.5281/zenodo.23556292
UR - https://zenodo.org/records/23556292
AB - We investigate whether a multiflavor fermionic pregeometric framework can dynamically select a single composite tetradic condensate from competing flavor channels. Within a leading projected ladder/large-N functional-renormalization-group truncation, we analyze a J = 2 channel whose dimensionless coupling obeys βg = 4g − ATg2, with AT > 0 under the physical transverse-traceless susceptibility prescription adopted in the truncation. The corresponding critical separatrix is g∗ = 4/AT. A flavor-dependent splitting permits the win dow gS > g∗ >gA, so that the flavor singlet reaches the collective instability while a positive subcritical adjoint branch remains below criticality. In the bosonized branch considered here, singlet criticality is compatible with a nonzero tetradic condensate while the flavor-adjoint directions retain positive quadratic curvature, yielding an operationally monometric phase within the truncation. For a Hermitian physical transverse-traceless spin-2 channel with nonzero spectral support and a well-defined subtracted dispersive representation, Källén Lehmann positivity implies Zdisp TT > 0. This result fixes only the dispersive contribution; it does not determine local matching terms, the complete renormalized Planck coefficient, or the full pole structure of the theory. The construction therefore provides a conditional dynamical mechanism for selecting a single tetradic background from a multiflavor fermionic system rather than a derivation of complete general relativity. Full Ward identities, local matching, torsional dynamics, ghost tests outside the TT sector, and nonlinear completion remain open problems for subsequent stages of the B-MECG research program
ER -