Dark energy
An optical effect
In DFD the dimming of distant supernovae comes from light crossing the ψ field on its way to us, which v4.0 calls a ψ-screen, rather than from a universe whose expansion is speeding up.
A guide to Density Field Dynamics
What if gravity isn’t curved spacetime, but a medium where light slows down near mass? This guide walks through the idea, the tests it has to pass, the numbers it claims to derive, and how it could be proven wrong. It takes about ten minutes.
Chapter one · The problem
General Relativity has passed every test we have given it for more than a century. It explained Mercury’s orbit, predicted the bending of starlight, and forecast gravitational waves decades before anyone could detect them.
Yet when we use it to weigh the universe, the books don’t balance. The standard model of cosmology needs two ingredients that no one has ever seen directly.
In the standard picture, ordinary matter makes up about 5% of the universe. That includes every star, planet, and person. The rest is dark matter and dark energy. Both are inferred from how things move, and neither has been detected in a laboratory.
Stars far from a galaxy’s center should orbit slowly, the way the outer planets orbit the Sun slowly. They don’t. Measured speeds stay flat far past the point where the visible matter runs out.
Chapter two · The theory
Density Field Dynamics starts from a different picture. Space is flat, but it isn’t empty. It carries a field, ψ (psi), that grows near mass. Where ψ is larger, light travels more slowly, so its path bends, the way light bends through glass or shimmers over hot asphalt.
The same field tells matter how to fall. One field does the job that curved spacetime does in General Relativity.
The refractive index of space. Light’s local speed is c·e−ψ, so it slows and bends near mass.
The acceleration of a falling body. Matter slides down the slope of the same field.
How strongly ψ responds depends on how strong gravity already is. DFD’s response function is μ(x) = x / (1 + x), where x compares the local acceleration with a tiny scale, a⋆ = 2√α·cH₀, about 1.2 × 10⁻¹⁰ m/s². Slide it and watch the two regimes.
Continuous fit parameters. The v4.0 release fixes its constants from theory instead of tuning them to data. The theory predicts, or it fails.
Apply that one rule to the same galaxies, using only the stars and gas you can see. There is no dark matter halo and no galaxy-by-galaxy tuning. The same settings run for all five.
Any rival to General Relativity has to match it wherever it has already been tested. In the weak-field limit DFD reproduces all ten post-Newtonian parameters, with γ = β = 1, so the classic tests come out the same.
The extra 43 arcseconds per century of perihelion shift.
Starlight grazing the Sun bends by 1.75 arcseconds.
Radio signals slow near the Sun by the amount Cassini measured.
Clocks run slower deeper in a gravitational well, as GPS requires.
They travel at exactly c. In 2017 the gamma rays from a neutron-star merger arrived 1.7 seconds after its gravitational waves, after a 130-million-light-year trip.
No Nordtvedt effect: the Earth and the Moon fall toward the Sun alike.
Chapter three · The numbers
The v4.0 framework goes further than gravity. It attaches a small internal space to every point, CP² × S³, seven extra dimensions curled up far below the reach of any microscope. The papers argue that this shape is the only one consistent with a few basic requirements on the vacuum, and that the forces and particles of the Standard Model follow from it.
The fine-structure constant, α, sets the strength of electromagnetism. Its inverse is about 137, and no accepted theory explains why. DFD’s v4.0 papers give a closed-form expression built from whole numbers that come from the internal geometry.
“One of the greatest damn mysteries of physics.”Richard Feynman, on the number 137
With Tr(Y²) = 10, kmax = 60, Nsp = 7, gF = 8.
The same geometry is used to derive the masses of all nine charged fermions: the electron, muon, and tau, and the six quarks. The v4.0 release reports a 1.42% mean error across all nine, with no per-particle fitting.
Chapter four · The cosmos
Standard cosmology treats dark matter and dark energy as ingredients whose amounts are measured, not explained. DFD’s v4.0 release tries to derive both.
Dark energy
In DFD the dimming of distant supernovae comes from light crossing the ψ field on its way to us, which v4.0 calls a ψ-screen, rather than from a universe whose expansion is speeding up.
Dark matter
v4.0 includes a cold, collisionless component whose abundance, Ωχh² = 0.1182, is computed forward from topology instead of fitted. Planck measures about 0.120.
The cosmological-constant problem
The largest mismatch in physics, between the vacuum energy theory expects and what we observe, appears in DFD as a power of α, with no fine-tuning.
The Hubble tension
Measurements of the expansion rate disagree: about 67 from the early universe and about 73 from nearby stars. DFD’s v4.0 value is 72.09, within 0.3σ of the SH0ES and JWST measurements.
Chapter five · The verdict
A theory is only as good as the experiments that could kill it. DFD’s predictions are frozen and dated. Here is where it is exposed.
DFD requires gravitational waves to travel at exactly the speed of light.
DFD dies ifa difference is measured, even at one part in 10¹⁵.
DFD and General Relativity agree through second order and first differ at third. DFD predicts a shadow about 4.6% larger.
DFD dies ifnext-generation Event Horizon Telescope images match GR’s size.
DFD ties the galactic scale to the expansion rate, a⋆(z) = 2√α·cH(z), so it should have been larger in the early universe.
DFD dies ifa⋆ is found frozen at high redshift.
Nuclear clocks built on ²²⁹Th, cross-species atomic comparisons, and cavity–atom tests probe how ψ couples to light and matter.
DFD dies ifthose comparisons show none of the channel-resolved signals it predicts.
v4.0 publishes frozen predictions for Belle II, JUNO, KATRIN, LISA, and Euclid.
DFD dies ifresults land outside the stated ranges.
Every headline number in the v4.0 release can be rechecked. One command, python3 reproduce.py, recomputes them in about a minute and compares each with the value printed in the paper.
Einstein’s equations work. DFD asks whether the geometry behind them is the right picture, or a very good approximation of a simpler one. The experiments above will decide.
This guide summarizes Density Field Dynamics v4.0 (July 2026). All DFD papers are preprints.