PulseExploreJournal ClubDebatesTrendingResearchersJournals
Instagram
HomeExploreJournal ClubTrending
Synapse
⌘+K
Synapse
April 3, 20260 citationsOpen Access

Sub-threshold Modes Propagating under Effective Geometry in a Phase-Field Framework

View Full Paper
YNYann Nédélec

Key Points

  • The aim is to examine how effective geometry influences the propagation of sub-threshold modes in a phase-field framework.
  • Identified effective geometry through Madelung decomposition of a complex scalar field.
  • Developed a theoretical model predicting mode behavior under specific wavelength conditions.
  • Conducted numerical simulations to assess energy transport directionality.
  • Three exact conditions characterizing the window boundary structure were established.
  • Simulations showed a +7% to +14% increase in energy transported rightward across the sub-threshold window.
  • The upper boundary's group velocity was confirmed to equal √2.

Abstract

Sub-threshold Modes Propagating under Effective Geometry in a Phase-Field Framework Yann Patrick Marie NÉDÉLEC — 31 March 2026 This note identifies a falsifiable prediction of the effective geometry gₑff = Ω² (x) ·η associated with a complex scalar field in its Madelung decomposition. The effective geometry reduces the local mass to mₑff (x) = m·Ω (x). Under a WKB non-singularity condition at the Planck epoch (σ₀ = 1/ (m√2) ), modes whose wavelength lies in the window λC < λ < √2·λC are evanescent on flat Minkowski spacetime but become propagating in the central region under gₑff. This window is universal relative to the Compton wavelength and depends only on the WKB hypothesis. Three exact results characterise the window boundary structure, all following from the single condition Ω² (0) = 1/2: (i) the group velocity at the upper boundary equals √2 exactly; (ii) the maximum frequency within the window is m/√2; (iii) the frequency vanishes at the lower boundary, indicating a threshold mode of vanishing frequency at the onset of propagation. The observable Eᵣight/Eₜotal (fraction of energy transported rightward) provides a clean, regularization-independent test. Numerical simulation gives Δ (Eᵣight/Eₜotal) = +7% to +14% across the full sub-threshold window k ∈ (m·Ω (0), m). The mechanism differs from standard analogue gravity models (Unruh 1981; Visser 1998; Barceló, Liberati and Visser 2005), where the effective metric is induced by fluid flow velocity. Here, Ω² (x) arises directly from the Madelung quantum potential of the background field. The acoustic analogy provides physical intuition only; the central result rests on the dispersion relation and the numerical scan. Limits are explicitly stated: frozen-background approximation, window width conditional on the WKB hypothesis, and absolute scale dependent on m (not fixed without the coupling constant κ). This note is extracted from Triptyque Conceptuel (Conceptual Triptych) v7, Y. P. M. NÉDÉLEC (2026), Zenodo, DOI: 10. 5281/zenodo. 19355673.

Ask AI
Helpful
Bookmark
Share
View Full Paper

Cite This Study

Yann Nédélec (2026) studied this question.

synapsesocial.com/papers/69cf5f005a333a821460dd6ahttps://doi.org/10.5281/zenodo.19356179
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. 1Effective mass of a spatially structured mode of the electromagnetic field: a single invariant for the group-velocity defect and the radiation-pressure defect2026
  2. 2A Threshold Model for Quantum-Classical Duality: Wave and Particle State as Binary Expressions of a Unified Fundamental Field2026
  3. 3HγC W6: A First Schrödinger-Type Effective Description for Near-Critical Fluctuation Modes2026 · 10 citations
  4. 4Quantum Fluctuation Energy from a Temporal Substrate: A Self-Contained First-Principles Derivation via Spontaneous Frame Selection, Wilsonian Effective Field Theory, and Harmonic Vacuum Structure2026
  5. 5QM and GR as Two Regimes of One Dissipative Dynamics. Quantum Mechanics and General Relativity As two Regimes of One Dissipative Dynamics2026