PulseExploreJournal ClubDebatesTrendingResearchersJournals
Instagram
HomeExploreJournal ClubTrending
Synapse
⌘+K
Synapse
February 25, 20260 citationsOpen Access

Heisenberg-Type Uncertainty from Scale–Translation Weyl Pairs in SU(N)-Covariant Time–Scalar Spectral Geometry

View Full Paper
JFJordan Gabriel Farrell

Key Points

  • The research aims to identify a Heisenberg-type uncertainty structure inherent to the SU(N)-covariant Time–Scalar Field Theory framework.
  • Developed the covariant operator and demonstrated holonomy-controlled Floquet sectorization.
  • Derived Bohr-type discretization via monodromy closure.
  • Investigated the scale-position operator and unitary scale-translation operator using the cell Hilbert space ℓ²(Z;Cⁿᵖ).
  • Established an exact Weyl commutation relation between operators.
  • Demonstrated the canonical conjugate pair generated by discrete scale translation.
  • Shown that the derived Weyl structure generates a rigorous scale-phase uncertainty bound.
  • Indicated that localization along the TSFT scale chain leads to delocalization in closure phase.

Abstract

We establish a Heisenberg-type uncertainty structure intrinsic to the SU (N) -covariant Time–Scalar Field Theory (TSFT) scale-chain framework. Building on prior work that constructed the covariant operator, demonstrated holonomy-controlled Floquet sectorization, and derived Bohrtype discretization via monodromy closure, we identify the canonical conjugate pair generated by discrete scale translation. Working on the cell Hilbert space ℓ² (Z;CNL), we prove that the scale-position operator and the unitary scale-translation operator satisfy an exact Weyl commutation relation. Under the Floquet transform, this pair is shown to be unitarily equivalent to the differential–multiplication duality (i∂κ, ; e^−iκ), where the closure phase κ is the spectral variable governing TSFT monodromy. From this Weyl structure we derive a rigorous scale–phase uncertainty bound, demonstrating that strong localization along the TSFT scale chain necessarily induces delocalization in closure phase. This provides the Heisenberg-type complement to the previously established Bohr discretization mechanism. The result completes the minimal operator-theoretic backbone of the TSFT spectral program: covariant construction, holonomy sectorization, boundary-induced quantization, and canonical conjugacy. No particle identification is asserted; the work is purely structural.

Ask AI
Helpful
Bookmark
Share
View Full Paper

Cite This Study

Jordan Gabriel Farrell (2026) studied this question.

synapsesocial.com/papers/699e91d7f5123be5ed04fad4https://doi.org/10.5281/zenodo.18743056
Ask AI
Helpful
Bookmark
Share
View Full Paper

Also Consider

Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context:

  1. 1Bohr Quantization from Monodromy Closure in SU(N)-Covariant Time–Scalar Spectral Geometry2026
  2. 2Holonomy and Floquet Sectorization in SU(N)-Covariant Time–Scalar Spectral Geometry2026
  3. 3Dirac Spinor Emergence from First-Order Factorization in SU(2)-Covariant Time–Scalar Spectral Geometry2026
  4. 4Schrödinger Dynamics as the Low-Spectrum Limit of SU(N)-Covariant Time–Scalar Spectral Geometry2026
  5. 5A Spectral Mechanism for Hierarchical Mass Emergence in Time-Scalar Field Theory2026