8. QUANTUM MECHANICS: EMERGENT HYDRODYNAMICS
8. QUANTUM MECHANICS: EMERGENT HYDRODYNAMICS
We reject:
Observer-dependent reality (Copenhagen interpretation)
Wavefunction collapse as fundamental (von Neumann)
Nonlocality as fundamental (EPR spookiness)
We assert:
Quantum phenomena are hydrodynamic effects of the vacuum substrate
Uncertainty is pixelation (finite grain size)
Entanglement is geometric (bulk connectivity)
Measurement is physical interaction (not consciousness)
Heisenberg: $$\Delta x \cdot \Delta p \geq \frac{\hbar}{2}$$
SBF Interpretation: This is the diffraction limit of the vacuum lattice, not a fundamental mystery.
8.2.1 Position Uncertainty (The Pixel)
The vacuum has finite grain size L_P. You cannot define position more precisely than: $$\Delta x \geq L_P$$
Mechanism: Localizing a knot to Δx < L_P requires displacing multiple grains simultaneously against bulk modulus K.
Energy Cost: $$E_{localize} \approx K (\Delta x)^3 / L_P^2$$
For Δx → 0, energy diverges.
8.2.2 Momentum Uncertainty (Thermal Kick)
The restoring force from compression fluctuates thermally (vacuum zero-point motion): $$\Delta p \approx \frac{k_B T_{vac}}{\Delta x} \approx \frac{\hbar c}{L_P \cdot \Delta x}$$
For Δx ≈ L_P: $$\Delta p \approx \frac{\hbar c}{L_P^2} = \frac{\hbar}{L_P} \times c$$
Product: $$\Delta x \cdot \Delta p \approx L_P \cdot \frac{\hbar}{L_P} = \hbar \quad \checkmark$$
Result: Uncertainty principle emerges from:
Discrete lattice (position limit)
Thermal fluctuations (momentum kick)
No wavefunction collapse needed
Double-Slit Experiment:
Standard QM: Particle is in superposition of going through both slits simultaneously.
SBF: Particle goes through ONE slit, but creates a bow wave (pressure field) that goes through BOTH slits and interferes.
8.3.1 The Pilot Wave Mechanism
Knot moves → displaces grains → generates phonon pressure field (bow wave)
Bow wave propagates ahead at speed c
Wave passes through both slits, interferes on far side
Standing pressure pattern forms (high/low density zones)
Particle exits one slit, encounters turbulence
Particle "surfs" into low-pressure zones (interference troughs)
Result: Interference pattern without particle splitting.
This is physical, not probabilistic.
8.3.2 Decoherence (The Detector)
Placing detector at slit:
Injects energy into vacuum
Disrupts delicate bow wave (turbulence)
Destroys coherent interference pattern
Particle reverts to ballistic trajectory
No wavefunction collapse - just hydrodynamic disruption.
8.3.3 Comparison with de Broglie-Bohm
Similarities:
Both have pilot wave guiding particle
Both are deterministic
Both reproduce standard QM predictions
Difference:
Bohm: Wave is abstract (ψ-field in configuration space)
SBF: Wave is physical (phonon pressure in real space)
Connection to Standard Formalism: This hydrodynamic model provides the physical substrate for Nelson's Stochastic Mechanics (1966). Nelson demonstrated that the Schrödinger equation can be rigorously derived from Newtonian mechanics, provided particles are subject to a specific background Brownian motion. SBF identifies this background not as an arbitrary mathematical assumption, but as the thermal fluctuations of the granular vacuum grains ($T_{vac} \approx c/L_P$). Thus, the Schrödinger equation is the emergent description of granular hydrodynamics.
SBF advantage: Makes additional prediction - wave speed should equal c (testable with ultra-precise interferometry).
EPR Paradox: Measuring spin of particle A instantly determines spin of particle B, even if separated by light-years.
Standard Interpretations:
Copenhagen: Nonlocal wavefunction collapse (magic)
Many-worlds: Branching realities (untestable)
Pilot wave: Nonlocal potential (action at distance)
SBF Interpretation: Particles are geometrically connected through 11D bulk.
8.4.1 The Flux Tube Model
Axiom: Entangled particles A and B are not separate objects. They are the two endpoints of a single U-shaped flux tube extending through higher-dimensional bulk.
Structure:
Contact network (3D brane) = where we observe particles
Bulk (11D) = where flux tube resides
Endpoints = where tube anchors to brane
Key Property: The flux tube is rigid (stiffness G_bulk >> G_brane).
8.4.2 Measurement as Boundary Constraint
Process:
Detector at angle θ_A measures particle A
Measurement imposes boundary condition on flux tube endpoint
Because tube is rigid, constraint propagates through bulk
Endpoint B's orientation is geometrically determined
Detector at angle θ_B measures the projected orientation
Critical Insight: There is no "signal" traveling from A to B in 3D space. Both measurements couple to the same bulk object simultaneously.
Analogy: Pushing one end of a rigid rod instantly affects the other end - not because information travels along the rod, but because the rod is a single object.
8.4.3 Mathematical Formulation
The Correlation Function:
For measurements at angles θ_A and θ_B: $$E(\theta_A, \theta_B) = -\cos(\theta_A - \theta_B)$$
Derivation:
Let flux tube orientation in bulk be V⃗. Measurement "snaps" V⃗ to align with θ_A (at endpoint A).
Due to antipodal constraint, endpoint B points at θ_A + π.
Detector B measures projection: $$P(B_\uparrow | A_\uparrow) = \cos^2\left(\frac{\theta_B - (\theta_A + \pi)}{2}\right) = \sin^2\left(\frac{\theta_A - \theta_B}{2}\right)$$
Correlation: $$E = -\cos(\theta_A - \theta_B) \quad \checkmark$$
This reproduces quantum mechanics exactly.
8.4.4 Why This Evades Bell's Theorem
Bell's Theorem: No local hidden variable theory can reproduce quantum correlations.
SBF Response: The flux tube orientation V⃗ is contextual (depends on measurement configuration θ_A, θ_B), not predetermined at creation.
This is allowed by Bell - contextual hidden variables can violate Bell inequalities.
Key: V⃗ is determined BY the measurement setup, not BEFORE it. This is geometric constraint satisfaction, not causal signaling.
8.4.5 Unique Prediction: The Entanglement Binding Energy
Unlike standard Quantum Mechanics, which treats entanglement as a purely informational correlation, SBF predicts that the connecting flux tube carries a physical energy cost.
The Mechanism (Vacuum Tension):
The flux tube is a region of higher geometric stiffness (tension) within the bulk vacuum. To satisfy energy conservation, this tension manifests as a binding energy subtracted from the local vacuum background.
Effective Mass: According to General Relativity ($E=mc^2$), this localized energy density creates a gravitational anomaly.
Magnitude: The effective mass scales with the tube length $d$ (stretching the vacuum) and the Planck stiffness:
$$M_{tube} \approx \pm \frac{\hbar}{c^2} \cdot \frac{d}{L_P}$$
Note: The sign ($\pm$) depends on the specific metric signature of the bulk-brane interface; a tension typically manifests as a positive effective mass in the weak-field limit.
Quantitative Prediction:
For a satellite-scale entanglement experiment ($d = 1000$ km):
$$M_{tube} \approx 10^{-18} \text{ kg} \quad (\approx 1000 \text{ electron masses})$$
Detection Strategy:
This is a measurable gravitational perturbation, not a new particle.
Setup: Entangle macroscopic test masses (optomechanical oscillators, $10^{-10}$ kg).
Measurement: Monitor for transient gravitational gradients along the line of sight during entanglement swapping.
Falsification: If high-precision gravimeters ($10^{-12}$ g sensitivity) detect no mass anomaly associated with the entanglement link, the physical flux tube model is falsified.
Barrier Penetration:
Standard QM: Wavefunction exponentially decays into classically forbidden region.
SBF: Particle traverses void network via percolation paths.
8.5.1 The Mechanism
Potential Barrier = Region of High Contact Density:
In SBF, potential V(x) maps to packing fraction φ(x): $$V(x) \propto \phi(x)$$
High potential = dense packing (few voids)
Thermal Fluctuations:
The vacuum undergoes zero-point motion. These fluctuations constantly open/close interstitial pores.
Tunneling Event:
Random fluctuation opens a percolation path (chain of connected voids) through the barrier region.
Particle (knot) squeezes through a temporary path.
Path closes after particle passes.
8.5.2 Tunneling Probability
Derivation:
Probability of opening path of length L through barrier: $$P_{tunnel} \propto \exp\left(-\frac{N \cdot V_{barrier}}{k_B T_{vac} \cdot \epsilon}\right)$$
where:
N = knot complexity (crossing number)
V_barrier = barrier height (excess coordination)
ε = void ratio = (φ_max - φ)/φ_max
T_vac = ℏc/L_P (vacuum temperature)
This reproduces WKB approximation structure (exponential suppression).
Unique Prediction:
Tunneling rate should decrease faster than expected for composite particles (high N), because complexity enters linearly, not as √m.
Test: Precision tunneling measurements with molecules vs atoms.