PulseExploreJournal ClubDebatesTrendingResearchersJournals
Instagram
HomeExploreJournal ClubTrending
Synapse
⌘+K
Synapse
May 28, 20260 citationsOpen Access

Discrete-to-Continuous Phase Transport Theorem

View Full Paper
CHCraig Edwin HoldwayResearch Manitoba

Key Points

  • This theorem aims to bridge the gap between discrete and continuous phase transport in quantum systems.
  • Uses the near-identity transport form to derive the relationship between discrete and continuous transport.
  • Proves convergence of iterated discrete transport to continuous exponential phase evolution.
  • Analyzes the structural importance of the decomposition of the transport operator.
  • Establishes that iterated discrete transport converges to continuous phase evolution as described by the identity e^{tA}=Icos(t) + Asin(t).
  • Confirms the robustness of the convergence under specified assumptions for the discrete transport operator.
  • Highlights the connection between discrete transport and the rotational generator for the coarse Z8 barrier cycle.

Abstract

T80 establishes the discrete-to-continuous phase transport bridge for the reduced defect-sector transport operator. Starting from the near-identity transport form₏₇₀ₒ₄=I+ A+O (²), ²=-I, theorem proves that iterated discrete transport converges to continuous exponential phase evolution: ₏₇₀ₒ₄ᵏ^tA=I t + A t, =k. \ The theorem is structurally important because it provides the canonical analytic mechanism connecting discrete barrier iteration to continuous sinusoidal phase flow within the Q5 reduced transport sector. T80 strengthens the T64-T65 emergent-generator arc by showing that repeated discrete transport naturally generates a continuous unitary phase evolution governed by the same rotational generator responsible for the coarse \ (Z₈\) barrier cycle. The decomposition^tA=I t + A t diagonal retention structure from rotational pass-through structure and links directly to the extraction and admissibility framework developed in T26-T29. Status: solid for the convergence₏₇₀ₒ₄ᵏ^tA the stated assumptions and for the closed-form identity^tA=I t + A t; for the identification of the full raw barrier transport operator with the isolated phase transport sector prior to the canonical projection result deferred to T81.

Ask AI
Helpful
Bookmark
Share
View Full Paper

Cite This Study

Craig Edwin Holdway (2026) studied this question.

synapsesocial.com/papers/6a17dcdf3fad632b0f9d9972https://doi.org/10.5281/zenodo.20400113
Ask AI
Helpful
Bookmark
Share
View Full Paper