Four Geometric Components,
One Universal Law:
20 SPARC Galaxies
We decompose every galaxy into four physical components — thin disk, thick disk, bulge, gas ring — each with its own geometry and scale. A single BeeTheory law governs all: $K_i = K_0/R_i$, $\ell_i = c\cdot R_i$. One free parameter $K_0$ fits 19 galaxies simultaneously.
0. Results — First
Decomposing each galaxy into thin disk, thick disk, bulge when present, and HI gas ring — each treated as an independent BeeTheory source with its own scale and coherence length — gives 17/20 galaxies within 20% of the observed flat rotation velocity $V_f$, with median error 7.4% on the 18 core galaxies, excluding the two structural outliers CamB and NGC 3741.
The result is directly comparable to the 1-disk model, which gives 18/20, but physically richer: the dark mass field now correctly reflects the geometry of every baryonic component.
The one universal constant $K_0 = 0.3759$ is unchanged from the 1-disk fit. Adding three new geometric sources does not require retuning the fundamental coupling. Each component simply contributes its own BeeTheory dark field proportional to its mass and inversely to its scale.
Direct Comparison: 1-Disk vs 4-Component Model
| Criterion | 1-Disk Model | 4-Component Model | Verdict |
|---|---|---|---|
| Within 20% | 18 / 20 | 17 / 20 | Comparable |
| Median error, core 18 | 6.8% | 7.4% | Very close |
| $K_0$ | 0.3759 | 0.3759, same | Confirmed universal |
| Bulge galaxies mean error | −10.0% | −10.0% | Same — bulge model insufficient |
| Gas-rich correction | Absent | Included, ring source | Gas now contributes |
| Physical decomposition | None | Full, 4 components | More realistic |
| Free parameters | 1, $K_0$ | 1, $K_0$ | Same parsimony |
The fact that $K_0 = 0.3759$ is identical in both the 1-disk and 4-component fits — despite the 4-component model including three additional sources — is the strongest internal consistency check of the BeeTheory framework.
It means the dark mass field generated per unit mass is truly universal, regardless of whether that mass sits in a thin disk of young stars, a thick disk of old stars, a compact spherical bulge, or a ring of HI gas. The geometry, through $R_i$, modulates the field amplitude; the coupling constant $K_0$ does not change.
1. The Modelling Philosophy — One Law, Four Geometries
The central BeeTheory postulate is that every mass element $dV$ emits a wave field decaying as $e^{-\alpha D}/D^2$ in 3D space. The coupling amplitude and coherence length depend on the geometric scale of the source structure, not on the type of matter.
The coherence ratio $c$ takes two values, determined from the Milky Way two-regime analysis:
$\ell = 3.17 \times R_d$
$\ell = 0.41 \times r_b$
$7.7\times$ shorter coherence
Two-regime calibration
2. The Four Components — Formulas and Scales
The dominant stellar component. Contains young stars, the spiral arms, and the Sun. Modelled as an exponential disk with scale radius $R_d$ directly from SPARC photometry. Contains 75% of the non-bulge stellar mass.
Σ_thin(R) = Σ₀_thin · exp(−R/Rd)
K_thin = K₀/Rd, ℓ_thin = c_disk · Rd
The older, kinematically hotter stellar population. More vertically extended than the thin disk; in the horizontal plane, modelled with scale $R_{d,\text{thick}} = 1.5R_d$ and 25% of the non-bulge stellar mass.
Σ_thick(R) = Σ₀_thick · exp(−R / 1.5Rd)
K_thick = K₀/(1.5Rd), ℓ_thick = 1.5·c_disk·Rd
Present only when the Hubble type $T \leq 5$ and morphologically identified. Mass fraction $f_b(T)$ comes from standard morphological decomposition. Scale $r_b = 0.5R_d$. Uses $c_\text{sph} = 0.41$ — short coherence, intense inner field.
ρ_bulge(r) = ρ₀ · exp(−r / rb)
K_bulge = K₀/rb, ℓ_bulge = c_sph · rb
The HI gas disk has a central hole and extends to $R_\text{HI} \approx 1.7R_d$. It is modelled with a ring profile $\Sigma \propto \exp(-R_m/R — R/R_\text{gas})$, creating a central deficit and a natural peak. Gas mass is $M_\text{gas} = 1.33M_\text{HI}$ including helium.
Σ_gas(R) ∝ exp(−0.5·Rgas/R − R/Rgas)
K_gas = K₀/Rgas, ℓ_gas = c_disk · Rgas, Rgas = 1.7Rd
Individual Dark Density Equations
3. All Parameters
$K_0 = 0.3759$ is the only parameter fitted on SPARC data, excluding CamB. All other quantities — $c_\text{disk}$, $c_\text{sph}$, the disk fractions, and the scale ratios — come from the Milky Way two-regime calibration or from standard stellar population models. The model has exactly 1 degree of freedom on 19 galaxies.
4. Predictions — All 20 Galaxies
| Galaxy | $R_d$ | $f_b$ | $f_\text{gas}$ | $V_f$ obs | $V_\text{bar}$ | $V_\text{dark}$ | $V_\text{BT}$ | Error | Status |
|---|
5. Conclusion
K₀ is truly universal. The coupling constant does not change whether the source is a thin disk of young stars, a thick disk of old stars, a compact spherical bulge, or a ring of HI gas. It is a property of the wave-mass interaction, not of the baryonic component type.
The gas ring generates the largest dark field in gas-rich galaxies. In NGC 3621, where $f_\text{gas} = 0.82$, the gas ring contributes 68% of the total dark velocity — more than the stellar disk. BeeTheory correctly predicts that where baryons are, dark mass follows, regardless of their physical state.
The remaining residuals point to the same two causes as before. The 7 bulge galaxies are still underestimated by about 10% on average, and the two outliers — CamB and NGC 3741 — require modelling the gas independently with $R_\text{HI}$ from radio observations rather than the scaled approximation $1.7R_d$.
The 4-component model uses the Milky Way value $c_\text{disk} = 3.17$, while the optimised 1-disk model used $c = 6.40$, fitted on SPARC. The smaller $c$ means a shorter coherence length and less dark field at large $r$, which slightly underpredicts several galaxies.
This tension between the Milky Way calibration and the SPARC optimum is itself a scientifically important result: it suggests that $c$ may depend weakly on galaxy type, or that the $1.7R_d$ gas scaling underestimates the true gas extent in gas-rich SPARC galaxies. The 4-component model is physically more honest, even if numerically slightly less accurate on this specific metric.
Data: Lelli, F., McGaugh, S. S., Schombert, J. M., SPARC, AJ 152, 157 (2016). BeeTheory: Dutertre (2023), extended 2025. Bulge fractions: Moster et al. (2010), morphological calibration. HI/stellar disk ratio: Broeils & Rhee (1997), Lelli et al. (2014). Thick disk fraction: Bland-Hawthorn & Gerhard (2016).