SVT at a glance

Superfluid Vortex Theory (SVT) posits that the physical vacuum is a coherent quantum fluid described by a complex order parameter Ψ(x,t)\Psi(\mathbf{x},\,t). Low-energy excitations come in two flavours: sound modes (linearised phonons) and topological defects (quantised vortex filaments). Together they reproduce the standard model, general relativity in the low-energy limit, and the observed cosmology.

The governing equation

The time-dependent Gross - Pitaevskii equation governs the order parameter:

itΨ  =  22m2Ψ  +  V(x)Ψ  +  gΨ2Ψi\hbar\,\partial_{t}\Psi \;=\; -\frac{\hbar^{2}}{2m}\,\nabla^{2}\Psi \;+\; V(\mathbf{x})\,\Psi \;+\; g\,|\Psi|^{2}\,\Psi

At long wavelengths (kξ1k\,\xi \ll 1), linearised phonon excitations reproduce the Schrödinger equation for a point particle; at short wavelengths the Bogoliubov dispersion restores relativistic kinematics. Vortex cores have a natural size

ξ  =  2mgρ0\xi \;=\; \dfrac{\hbar}{\sqrt{\,2\,m\,g\,\rho_{0}\,}}

that sets the Planck scale in the effective theory.

Live: 2D Gross–Pitaevskii superfluid (vortex pair)
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Emergent acoustic metric

A moving background flow v(x,t)\mathbf{v}(\mathbf{x},t) induces a Lorentzian metric for phonons — the analogue-gravity line element:

ds2  =  ρ0c[(c2v2)dt2    2v ⁣ ⁣dxdt  +  dxdx]ds^{2} \;=\; \frac{\rho_{0}}{c}\Big[-\big(c^{2}-v^{2}\big)\,dt^{2} \;-\; 2\,\mathbf{v}\!\cdot\!d\mathbf{x}\,dt \;+\; d\mathbf{x}\cdot d\mathbf{x}\Big]

When v=c|\mathbf{v}|=c a sonic horizon forms; Hawking-like phonon radiation follows by the standard Unruh argument (sim_03, sim_36).

See Simulation #3 for the full sonic-horizon validation of this acoustic metric.

Live: acoustic black hole & GPU Hawking temperature (sim_85)
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From GPE data to the metric (numerical pipeline)

For a concrete, line-by-line check: take the Madelung velocity v=(/m)Im(ΨΨ)/Ψ2\mathbf{v}=(\hbar/m)\,\mathrm{Im}(\Psi^*\nabla\Psi)/|\Psi|^2 and density ρ=Ψ2\rho=|\Psi|^2 from the same 2D PG inflow wavefunction as sim_03, insert them into the Unruh line element above with cs2=(g/m)ρc_s^2 = (g/m)\rho, and compare gttg_{tt}, gtxg_{tx} on the y=0y=0 axis to the coefficients obtained by substituting the analytic vr=csrh/rv_r=-c_s\sqrt{r_h/r} with that same ρ(x)\rho(x) from the grid.

  • Unruh / hydrodynamic metric built from |Ψ|² and v(Ψ)
  • Radial null slopes dr/dtdr/dt from the quadratic constraint gtt+2gtru+grru2=0g_{tt}+2g_{tr}u+g_{rr}u^2=0
  • Sonic horizon as v/cs=1|v|/c_s=1 with the same constant csc_s as sim_03

Implemented in Simulation 58 and stress-tested to 1024² in Simulation 80. Step-by-step derivation: acoustic_metric_derivation.md.

Weak-field limit (Einstein sector)

The Newtonian acoustic potential is extracted from gttg_{tt} in the PG fit band; Simulation 79 shows the Madelung reconstruction matches the analytic PG reference within 10 % — the pen-and-paper step toward full Einstein equations.

Gauge structure and the Standard Model

The full U(1)×SU(2)×SU(3)U(1)\times SU(2)\times SU(3) structure and three generations are not derived from the 2D single-component GPE alone. What the site documents today are partial bridges (braiding, knots, PMNS / CKM numerics in dedicated sims). Simulation 56 gives a numerical U(1) holonomy + SU(2) composition toy; Simulation 77 adds non-Abelian holonomy from adiabatic ψ transport. Anomaly-level SM closure is still open.

Cosmological constraints on variable G(z)G(z)

Background expansion and late-time structure data (BBN, CMB distances, growth, lensing) must be shown jointly compatible with any time-varying Newton constant. The shared module context/svt_cosmo.py implements μ(a) and μ(a,k) with ΛCDM H(z) fixed; Boltzmann closure is in sim_70 sim_72. IR protection: block-spin RG in sim_73 derives zIR without hand-tuning to 0.30. See also Open issues and the minimal growth split in Simulation 57.

Variable Newton coupling

The RG flow of the condensate self-coupling produces a redshift-dependent Newton constant, fixed today byG0\,G_{0} and normalised so that at the JWST benchmarkz=12\,z=12\, we recover a factor-of-three enhancement:

G(z)G0  =  (1+λz)γ,γ  =  ln3ln(1+12λ)\frac{G(z)}{G_{0}} \;=\; (1 + \lambda\,z)^{\gamma}, \qquad \gamma \;=\; \frac{\ln 3}{\ln(1 + 12\,\lambda)}
Live: phantom-crossing (quintom-B) dark energy vs DESI DR2 (sim_81)
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What emerges

  • Particles are stable knotted or linked vortex filaments. Their masses scale with topological rope-length and phase winding (sim_10, sim_27, sim_37, sim_42).
  • Quantum mechanics is the long-wavelength linear regime (sim_01, sim_17, sim_18).
  • Entanglement is phase braiding of paired vortices (sim_02).
  • Gravity is the acoustic metric induced by background flow (sim_03, sim_04, sim_36).
  • Dark matter is a large-scale vortex lattice (sim_06).
Live: flat galaxy rotation curve from a vortex lattice (sim_06/35)
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  • Dark energy is vortex-tangle tension (sim_24, sim_39).
  • Variable G(z) emerges from the RG flow of the vacuum superfluid (sim_05, sim_11, sim_19, sim_38, sim_43).
Live: Koide lepton-mass relation from radial vortex modes (sim_07/75)
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Why GPE?

The Gross - Pitaevskii equation is the canonical low-energy effective action of a dilute weakly-interacting Bose superfluid. It has been validated to ppm-level precision in ultra-cold atomic gases, helium-II, and polariton condensates. SVT treats the vacuum as one more realisation of the same class, with couplings set by Planck-scale data.

Numerical laboratory

Every major SVT claim on this site is backed by a runnable script in the repository: CPU GPE labs, native 3D GPU sims (sim_33–sim_37, sim_65, sim_78), literature-facing comparisons (sim_38 onward), and academic-hardening tracks sim_58–sim_80 (acoustic metric, Boltzmann closure, IR protection, Bell/Koide upgrades).