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Einstein 2.0: A Fluid-Dynamic Representation of Quantum and Relativistic Phenomena via Toroidal Higgs-Field Vortices

Mohammd Raeed Al-anssari

Published Jun 11, 2026• 0 citations
Publisher

Abstract

This final version of my theory incorporates quantum tunneling. Section 4.4: Deterministic Quantum Tunneling This section reclassifies quantum tunneling from a probabilistic outcome to a deterministic, aerodynamic phenomenon. By decoupling motion into intrinsic (precessional tumbling) and extrinsic (orbital) reference frames, we demonstrate that tunneling occurs only when the particle’s zero-density supercavitation wake fully projects across the barrier’s thickness. Consequently, what is traditionally interpreted as "tunneling probability" is revealed to be a precise, mechanical duty-cycle dictated by the alignment of these wake-steering mechanics.

DOI
10.5281/zenodo.20647827

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Demystifying Quantum Tunneling and Radioactive Half-Life: A Deterministic Hydrodynamic Model within the 4D Topological Resonant Fractal Continuum

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The Copenhagen interpretation of quantum mechanics relies on intrinsic stochasticity and probability amplitudes to explain phenomena such as quantum tunneling and radioactive decay. This paper challenges the paradigm of fundamental randomness by proposing a strictly deterministic, kinematic explanation grounded in the Topological Resonant Fractal Continuum (TRFC) theory. By modeling the universe as a four-dimensional (4D) barotropic, inviscid fluid, we redefine elementary particles as macroscopic topological vortices and potential barriers as localized gradients of acoustic impedance. Within this framework, quantum tunneling is not a probabilistic teleportation of a point particle, but the deterministic evanescent leakage of topological stress through a pressure barrier, facilitated by momentary phase-alignments with vacuum fluctuations. Furthermore, the radioactive half-life (T1/2) is demystified. An unstable isotope is modeled as an overpressurized vortex near the Rayleigh-Plateau instability threshold. Decay (bifurcation) occurs deterministically when the internal vibrational precursors of the vortex constructively interfere with the ambient acoustic noise (vacuum phonons) of the 4D continuum, momentarily releasing the hydrostatic clamp. Consequently, half-life is simply the macroscopic statistical average of vacuum turbulence interacting with a specific topological geometry, suggesting that radioactive decay rates can be technologically engineered.

•Mar 19, 2026•0 citations

Demystifying Quantum Tunneling and Radioactive Half-Life: A Deterministic Hydrodynamic Model and Calculation of 4D Vacuum Acoustic Noise within the TRFC Theory

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The Copenhagen interpretation of quantum mechanics relies on intrinsic stochasticity and probability amplitudes to explain phenomena such as quantum tunneling and radioactive decay. This paper challenges the paradigm of fundamental randomness by proposing a strictly deterministic, kinematic explanation grounded in the Topological Resonant Fractal Continuum (TRFC) theory. By modeling the universe as a four-dimensional (4D) barotropic, inviscid superfluid, we redefine elementary particles as macroscopic topological vortices and potential barriers as localized gradients of acoustic impedance. We demonstrate that quantum tunneling is not probabilistic teleportation, but a deterministic evanescent leakage of topological stress facilitated by phase-alignment with vacuum fluctuations. Furthermore, we redefine the radioactive half-life (T1/2) as the macroscopic statistical average of the interaction between ambient vacuum acoustic noise (vacuum phonons) and the structural limit of an overpressurized topological knot. Applying this model, we reverse-engineer empirical decay data for Uranium-238 and Polonium-212. The calculations reveal that the 4D vacuum acoustic noise exhibits a consistent effective energy (E0) on the order of tenths of an MeV at the subatomic scale, thereby providing quantitative empirical support for the hydrodynamic model of 4D space.

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Macroscopic Quantum Hydrodynamics: Transitioning to Deterministic Continuum Mechanics and the Scale-Invariance of the Superfluid Vacuum

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This monograph provides a deterministic, hydrodynamic foundation for Quantum Mechanics, replacing the probabilistic abstractions of the Copenhagen interpretation. By redefining the cosmic vacuum as a tangible, compressible Bose-Einstein Condensate (BEC), the abstract Schrödinger equation is mathematically mapped directly to the classical Euler fluid momentum equations via the Madelung Transformation. Through this hydrodynamic lens, wave-particle duality is physically resolved: a localized quantum droplet is mechanically steered by the acoustic pressure gradient of its own wake. The Heisenberg Uncertainty Principle is explicitly recontextualized as the irreducible variance of convective diffusion—a microscopic buoy subjected to the continuous turbulence of the vacuum's kinematic viscosity. Furthermore, quantum entanglement is modeled not as an abstract, non-local phenomenon, but as continuous longitudinal phononic resonance. Scaling these sub-atomic continuum mechanics to astrophysics, this framework replaces collisionless Dark Matter and stochastic planetary accretion with macroscopic acoustic nodes, viscous fluid drag, and deterministic tidal thresholds—recently validated by 2026 Chandra observations of pre-ignition EUV thermalization. Ultimately, this demonstrates that quantum mechanics is simply fluid dynamics operating at extreme limits of scale and viscosity.

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Deterministic Quantum Tunneling as Filamentous Phase Filtering 3D Pseudo-Spectral Fourier Evidence in MDA Continuum Mechanics.pdf

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This repository contains the complete computational source code (Python script optimized for high-performance mobile CPU execution) and mathematical proof for the non-probabilistic, deterministic simulation of the quantum tunneling effect under the Angular Phase-Shift Mechanics (MDA) and the Topological Growth Equation (EDSA). Utilizing a high-fidelity 3D Split-Step Fourier Method (SSFM) engine, we systematically dismantle the orthodox Copenhagen interpretation of tunneling as a stochastic, discontinuous "probability jump." Real-time high-resolution telemetry demonstrates that an accelerated quiral electron solitón (\(m_0 = 0.511\) MeV/\(c^{2}\)) encountering a rigid electrostatic overpressure barrier (\(V_{max} = 12.00\) MeV) undergoes a strictly continuous, isoentropic (\(dS/dt \equiv 0\)) topological phase transition. The telemetry monitors a localized quiral vortex stretching elastically into a dense network of sub-visibles phase-space filaments that filter mass-energy through the barrier variety. Upon boundary exit, the universal topological rigidity constant (\(\beta_{torsion} = 0.128768\)) executes a geometric packing compression, clean-reconstituting the spherical solitonic core at a maximum recorded coherent transmission fraction of \(54.19\%\) at frame 122. Residual energy trapped inside the barrier variety maps onto a perfectly flat, non-dissipative harmonic acoustic echo, providing raw empirical validation for fully geometric, unfragmented unified field theorie s.

•Oct 5, 2026•0 citations

S-Field Mediated Tunneling as Direct Experimental Evidence for the S-Domain

Petkov, Dimitar

S-Field Mediated Tunneling as Direct Experimental Evidence for the S-Domain (Unicode clean manuscript version) 1. Overview Quantum tunneling is traditionally interpreted as a purely probabilistic penetration of a potential barrier. However, several well-documented empirical signatures — including non-classical traversal times, phase discontinuities, and mass-independent transmission — suggest the involvement of a deeper mechanism not contained within 4D physics. Within the Unified Oscillatory–Informational S-Framework, tunneling emerges naturally as a temporary de-projection of a particle into the S-domain, followed by re-projection into the baryonic domain (B-space). This process is mediated by the dual S-oscillatory structure (sb and bs modes) that governs all baryonic matter. A particle tunnels because it does not cross the barrier inside B, but because it temporarily exists in S, where spatial metrics do not apply. Thus tunneling becomes one of the strongest direct experimental signatures of the S-field 2. The S-Oscillator and the Two Projection Modes (sb and bs) Every baryonic particle is represented as a two-phase S-oscillator: Φ(t) = (Φ_sb(t), Φ_bs(t)). Both modes share the same base frequency ω but differ by phase and orientation: Φ_sb(t) = A_sb exp(i ω t + i φ_sb) Φ_bs(t) = A_bs exp(i ω t + i φ_bs) with phase difference Δφ = φ_bs − φ_sb. The sb mode projects preferentially into baryonic 3+1 space (B-space). The bs mode projects preferentially into the higher-dimensional S-domain. The instantaneous orientation between B and S is determined by Δφ and the ratio of amplitudes: tan θ = A_bs / A_sb. Orientation rules: • Low energy → θ → 0 → sb dominates → stable B projection • High energy → θ → π/2 → bs dominates → shift toward S This dichotomy underlies mass stability, resonance behavior, and tunneling. 3. Energy-Dependent Couplings to B and S Define coupling coefficients describing which mode is expressed in which domain: C_sb→B(E) = exp(−E_s / E) C_sb→S(E) = 1 − C_sb→B(E) C_bs→S(E) = exp(−E_b / E) C_bs→B(E) = 1 − C_bs→S(E). Where: • E_s = characteristic S-activation threshold • E_b = baryonic binding energy • E = instantaneous kinetic or local potential energy. This directly encodes the rule: When energy is low, the sb peak enters B. When energy is high, the bs peak enters S. This is the simplest and most important dynamical law of the S-framework. 4. Projection Operators and Domain Transition Define projection operators: P_B Φ = C_sb→B Φ_sb + C_bs→B Φ_bs P_S Φ = C_sb→S Φ_sb + C_bs→S Φ_bs. These satisfy: P_B + P_S = 1 P_B P_S = 0. A tunneling event is represented as: P_B Φ → P_S Φ → P_B Φ. Meaning: Baryonic projection → S-domain → baryonic projection at a new spatial coordinate. This eliminates any need for a spatial path inside the barrier. 5. Barrier Interaction and S-Transfer When Φ encounters a potential barrier V(x), the sb (B-bound) component compresses, which induces a transfer of amplitude into the bs (S-oriented) component: dΦ_bs/dt = κ exp(−V/E) Φ_sb, where κ is the S-coupling constant. This transfer is the physical cause of tunneling: • compression reduces B-stability, • Δφ increases, • orientation θ rotates toward S, • a finite portion of Φ enters S. Inside S, spatial distance has no meaning, so the traversal time is independent of barrier width. 6. Tunneling Probability in the S-Framework The tunneling probability is the product of: 1. S-orientation probability during compression 2. S-coherence propagation 3. re-projection probability. Explicitly: T = |P_S Φ|² |P_B Φ_after|². Using the projection definitions: |P_S Φ|² = |C_sb→S A_sb exp(i φ_sb) + C_bs→S A_bs exp(i φ_bs)|². Since sb→S dominates under compression: T ≈ (1 − exp(−E_s / E))² exp(−2L / λ_S), where λ_S is the S-coherence characteristic length. Observations: The entire classical exponential dependence arises from S-coherence decay, not from 4D probabilistic wave leakage. • The first factor is purely S-orientational: the bs-mode activation. This is experimentally identical to quantum mechanics but conceptually much simpler and ontologically richer. 7. Traversal Time and the Hartman Effect In the S-domain there is no spatial metric. Thus the internal traversal time τ_S satisfies: τ_S = undefined or zero. Therefore: τ_total = τ_in + τ_out, and τ_total becomes independent of barrier width for sufficiently thick barriers. This is an exact explanation of the Hartman effect — a long-standing paradox in standard quantum mechanics. only S-phase geometry. It also resolves the “observer independence” issue: the process depends solely on S-orientation, not on measurement. 9. Why Tunneling Is Direct Evidence for the S-Field Standard QM cannot explain: • zero or undefined traversal time • barrier-thickness independence • identical tunneling for particles with different classical masses • phase discontinuities stronger than wavefunction continuity allows • the existence of tunneling at arbitrarily low energies. In the S-framework: All these come from a single source: temporary existence in S, where spatial extension is undefined. Thus tunneling is not just compatible with the S-field. It is one of the strongest direct signatures that baryonic matter is a projection of a higher-dimensional oscillatory structure. 10. Unified S-Equation of Tunneling The full dynamical equation integrating B and S propagation is: Φ(t + Δt) = P_B U_B Φ(t) + P_S U_S Φ(t), with: U_B = exp(−i H_B Δt / ℏ) U_S = exp(−i E_S Δt). Inside S there is only intrinsic phase, no Hamiltonian with spatial term. A tunneling event occurs when: P_S U_S P_B Φ ≠ 0. This is the precise mathematical definition of S-mediated tunneling.

•Dec 6, 2025•0 citations
This final version of my theory incorporates quantum tunneling. Section 4.4: Deterministic Quantum Tunneling This section reclassifies quantum tunneling from a probabilistic outcome to a deterministic, aerodynamic phenomenon. By decoupling motion into intrinsic (precessional tumbling) and extrinsic (orbital) reference frames, we demonstrate that tunneling occurs only when the particle’s zero-density supercavitation wake fully projects across the barrier’s thickness. Consequently, what is traditionally interpreted as "tunneling probability" is revealed to be a precise, mechanical duty-cycle dictated by the alignment of these wake-steering mechanics.
The Copenhagen interpretation of quantum mechanics relies on intrinsic stochasticity and probability amplitudes to explain phenomena such as quantum tunneling and radioactive decay. This paper challenges the paradigm of fundamental randomness by proposing a strictly deterministic, kinematic explanation grounded in the Topological Resonant Fractal Continuum (TRFC) theory. By modeling the universe as a four-dimensional (4D) barotropic, inviscid fluid, we redefine elementary particles as macroscopic topological vortices and potential barriers as localized gradients of acoustic impedance. Within this framework, quantum tunneling is not a probabilistic teleportation of a point particle, but the deterministic evanescent leakage of topological stress through a pressure barrier, facilitated by momentary phase-alignments with vacuum fluctuations. Furthermore, the radioactive half-life (T1/2) is demystified. An unstable isotope is modeled as an overpressurized vortex near the Rayleigh-Plateau instability threshold. Decay (bifurcation) occurs deterministically when the internal vibrational precursors of the vortex constructively interfere with the ambient acoustic noise (vacuum phonons) of the 4D continuum, momentarily releasing the hydrostatic clamp. Consequently, half-life is simply the macroscopic statistical average of vacuum turbulence interacting with a specific topological geometry, suggesting that radioactive decay rates can be technologically engineered.
The Copenhagen interpretation of quantum mechanics relies on intrinsic stochasticity and probability amplitudes to explain phenomena such as quantum tunneling and radioactive decay. This paper challenges the paradigm of fundamental randomness by proposing a strictly deterministic, kinematic explanation grounded in the Topological Resonant Fractal Continuum (TRFC) theory. By modeling the universe as a four-dimensional (4D) barotropic, inviscid superfluid, we redefine elementary particles as macroscopic topological vortices and potential barriers as localized gradients of acoustic impedance. We demonstrate that quantum tunneling is not probabilistic teleportation, but a deterministic evanescent leakage of topological stress facilitated by phase-alignment with vacuum fluctuations. Furthermore, we redefine the radioactive half-life (T1/2) as the macroscopic statistical average of the interaction between ambient vacuum acoustic noise (vacuum phonons) and the structural limit of an overpressurized topological knot. Applying this model, we reverse-engineer empirical decay data for Uranium-238 and Polonium-212. The calculations reveal that the 4D vacuum acoustic noise exhibits a consistent effective energy (E0) on the order of tenths of an MeV at the subatomic scale, thereby providing quantitative empirical support for the hydrodynamic model of 4D space.
This work is the nineteenth installment in the Time Field Theory (TFT) series, succeeding Time Field Theory XVIII: Entanglement, Common Phase Splitting, and the Local Interpretation of Bell Experiments. This work presents a fully transparent, first-principles physical framework with no black-box operations or uninterpreted postulates. All dynamical processes are derived deterministically from time-field axioms, with clear, traceable physical mechanisms at every step. Within the TFT framework, quantum tunneling is derived without reliance on conventional quantum mechanics or probabilistic interpretation. Two fundamental mechanisms are distinguished: (1) electric potential coupling responsible for phase modulation, interference, and tunneling attenuation; (2) mass/time-field gradient responsible for phase locking, measurement, and localization. Tunneling is interpreted as deterministic time-field splitting rather than probabilistic selection: a portion of the time-field oscillation is retained inside the barrier with real energy deposition, while the remainder transmits. The tunneling transmission coefficient is verified against experimental data and shows quantitative agreement. A 2025 observation of under-barrier recollision supports real interactions inside the barrier, consistent with TFT. This work contributes to the unification of gravity, special relativity, and quantum mechanics within a self-consistent, locally realistic, and fully transparent time-field dynamics framework.
This monograph provides a deterministic, hydrodynamic foundation for Quantum Mechanics, replacing the probabilistic abstractions of the Copenhagen interpretation. By redefining the cosmic vacuum as a tangible, compressible Bose-Einstein Condensate (BEC), the abstract Schrödinger equation is mathematically mapped directly to the classical Euler fluid momentum equations via the Madelung Transformation. Through this hydrodynamic lens, wave-particle duality is physically resolved: a localized quantum droplet is mechanically steered by the acoustic pressure gradient of its own wake. The Heisenberg Uncertainty Principle is explicitly recontextualized as the irreducible variance of convective diffusion—a microscopic buoy subjected to the continuous turbulence of the vacuum's kinematic viscosity. Furthermore, quantum entanglement is modeled not as an abstract, non-local phenomenon, but as continuous longitudinal phononic resonance. Scaling these sub-atomic continuum mechanics to astrophysics, this framework replaces collisionless Dark Matter and stochastic planetary accretion with macroscopic acoustic nodes, viscous fluid drag, and deterministic tidal thresholds—recently validated by 2026 Chandra observations of pre-ignition EUV thermalization. Ultimately, this demonstrates that quantum mechanics is simply fluid dynamics operating at extreme limits of scale and viscosity.
This repository contains the complete computational source code (Python script optimized for high-performance mobile CPU execution) and mathematical proof for the non-probabilistic, deterministic simulation of the quantum tunneling effect under the Angular Phase-Shift Mechanics (MDA) and the Topological Growth Equation (EDSA). Utilizing a high-fidelity 3D Split-Step Fourier Method (SSFM) engine, we systematically dismantle the orthodox Copenhagen interpretation of tunneling as a stochastic, discontinuous "probability jump." Real-time high-resolution telemetry demonstrates that an accelerated quiral electron solitón (m0=0.511m_0 = 0.511m0​=0.511 MeV/c2c^{2}c2) encountering a rigid electrostatic overpressure barrier (Vmax=12.00V_{max} = 12.00Vmax​=12.00 MeV) undergoes a strictly continuous, isoentropic (dS/dt≡0dS/dt \equiv 0dS/dt≡0) topological phase transition. The telemetry monitors a localized quiral vortex stretching elastically into a dense network of sub-visibles phase-space filaments that filter mass-energy through the barrier variety. Upon boundary exit, the universal topological rigidity constant (βtorsion=0.128768\beta_{torsion} = 0.128768βtorsion​=0.128768) executes a geometric packing compression, clean-reconstituting the spherical solitonic core at a maximum recorded coherent transmission fraction of 54.19%54.19\%54.19% at frame 122. Residual energy trapped inside the barrier variety maps onto a perfectly flat, non-dissipative harmonic acoustic echo, providing raw empirical validation for fully geometric, unfragmented unified field theorie s.
S-Field Mediated Tunneling as Direct Experimental Evidence for the S-Domain (Unicode clean manuscript version) 1. Overview Quantum tunneling is traditionally interpreted as a purely probabilistic penetration of a potential barrier. However, several well-documented empirical signatures — including non-classical traversal times, phase discontinuities, and mass-independent transmission — suggest the involvement of a deeper mechanism not contained within 4D physics. Within the Unified Oscillatory–Informational S-Framework, tunneling emerges naturally as a temporary de-projection of a particle into the S-domain, followed by re-projection into the baryonic domain (B-space). This process is mediated by the dual S-oscillatory structure (sb and bs modes) that governs all baryonic matter. A particle tunnels because it does not cross the barrier inside B, but because it temporarily exists in S, where spatial metrics do not apply. Thus tunneling becomes one of the strongest direct experimental signatures of the S-field 2. The S-Oscillator and the Two Projection Modes (sb and bs) Every baryonic particle is represented as a two-phase S-oscillator: Φ(t) = (Φ_sb(t), Φ_bs(t)). Both modes share the same base frequency ω but differ by phase and orientation: Φ_sb(t) = A_sb exp(i ω t + i φ_sb) Φ_bs(t) = A_bs exp(i ω t + i φ_bs) with phase difference Δφ = φ_bs − φ_sb. The sb mode projects preferentially into baryonic 3+1 space (B-space). The bs mode projects preferentially into the higher-dimensional S-domain. The instantaneous orientation between B and S is determined by Δφ and the ratio of amplitudes: tan θ = A_bs / A_sb. Orientation rules: • Low energy → θ → 0 → sb dominates → stable B projection • High energy → θ → π/2 → bs dominates → shift toward S This dichotomy underlies mass stability, resonance behavior, and tunneling. 3. Energy-Dependent Couplings to B and S Define coupling coefficients describing which mode is expressed in which domain: C_sb→B(E) = exp(−E_s / E) C_sb→S(E) = 1 − C_sb→B(E) C_bs→S(E) = exp(−E_b / E) C_bs→B(E) = 1 − C_bs→S(E). Where: • E_s = characteristic S-activation threshold • E_b = baryonic binding energy • E = instantaneous kinetic or local potential energy. This directly encodes the rule: When energy is low, the sb peak enters B. When energy is high, the bs peak enters S. This is the simplest and most important dynamical law of the S-framework. 4. Projection Operators and Domain Transition Define projection operators: P_B Φ = C_sb→B Φ_sb + C_bs→B Φ_bs P_S Φ = C_sb→S Φ_sb + C_bs→S Φ_bs. These satisfy: P_B + P_S = 1 P_B P_S = 0. A tunneling event is represented as: P_B Φ → P_S Φ → P_B Φ. Meaning: Baryonic projection → S-domain → baryonic projection at a new spatial coordinate. This eliminates any need for a spatial path inside the barrier. 5. Barrier Interaction and S-Transfer When Φ encounters a potential barrier V(x), the sb (B-bound) component compresses, which induces a transfer of amplitude into the bs (S-oriented) component: dΦ_bs/dt = κ exp(−V/E) Φ_sb, where κ is the S-coupling constant. This transfer is the physical cause of tunneling: • compression reduces B-stability, • Δφ increases, • orientation θ rotates toward S, • a finite portion of Φ enters S. Inside S, spatial distance has no meaning, so the traversal time is independent of barrier width. 6. Tunneling Probability in the S-Framework The tunneling probability is the product of: 1. S-orientation probability during compression 2. S-coherence propagation 3. re-projection probability. Explicitly: T = |P_S Φ|² |P_B Φ_after|². Using the projection definitions: |P_S Φ|² = |C_sb→S A_sb exp(i φ_sb) + C_bs→S A_bs exp(i φ_bs)|². Since sb→S dominates under compression: T ≈ (1 − exp(−E_s / E))² exp(−2L / λ_S), where λ_S is the S-coherence characteristic length. Observations: The entire classical exponential dependence arises from S-coherence decay, not from 4D probabilistic wave leakage. • The first factor is purely S-orientational: the bs-mode activation. This is experimentally identical to quantum mechanics but conceptually much simpler and ontologically richer. 7. Traversal Time and the Hartman Effect In the S-domain there is no spatial metric. Thus the internal traversal time τ_S satisfies: τ_S = undefined or zero. Therefore: τ_total = τ_in + τ_out, and τ_total becomes independent of barrier width for sufficiently thick barriers. This is an exact explanation of the Hartman effect — a long-standing paradox in standard quantum mechanics. only S-phase geometry. It also resolves the “observer independence” issue: the process depends solely on S-orientation, not on measurement. 9. Why Tunneling Is Direct Evidence for the S-Field Standard QM cannot explain: • zero or undefined traversal time • barrier-thickness independence • identical tunneling for particles with different classical masses • phase discontinuities stronger than wavefunction continuity allows • the existence of tunneling at arbitrarily low energies. In the S-framework: All these come from a single source: temporary existence in S, where spatial extension is undefined. Thus tunneling is not just compatible with the S-field. It is one of the strongest direct signatures that baryonic matter is a projection of a higher-dimensional oscillatory structure. 10. Unified S-Equation of Tunneling The full dynamical equation integrating B and S propagation is: Φ(t + Δt) = P_B U_B Φ(t) + P_S U_S Φ(t), with: U_B = exp(−i H_B Δt / ℏ) U_S = exp(−i E_S Δt). Inside S there is only intrinsic phase, no Hamiltonian with spatial term. A tunneling event occurs when: P_S U_S P_B Φ ≠ 0. This is the precise mathematical definition of S-mediated tunneling.