Extended Derivation of the Proton Superfluid Model (PSM)
The base PSM derives from superfluid quantization, where the proton's mass-radius relation satisfies \( r = \frac{n \hbar}{m c} \) with \( n=4 \) for the proton (\( m_p c^2 = 938.272 \) MeV, \( r_p \approx 0.841 \) fm), yielding an exact match. Correlations extend to other particles by assuming a similar effective radius, leading to \( m = \frac{n}{4} m_p \), with integer \( n \) and matches within 5% error, accounting for spectral broadening in resonances (widths Γ up to hundreds of MeV due to mixing or modulation).
To extend the model as requested, we incorporate additional quantum numbers analogous to those in mainstream quantum mechanics (e.g., hydrogen atom: principal \( n \), orbital \( l \), magnetic \( m \)), but adapted to particle physics with a "golden" quantum number \( k \) to allow fractional contributions via powers of the golden ratio \( \phi = \frac{1 + \sqrt{5}}{2} \approx 1.618 \). This is motivated by appearances of \( \phi \) in quantum physics literature, including Schrödinger equation energy-mass ratios, fine-structure constant relations, quark mass ratios (e.g., bare d/u ≈ φ), lepton mass patterns, and potential quasicrystal symmetries in hadron internals or E8 models.
The generalized effective quantum number is \( n_\text{eff} = n + \frac{l}{ \phi } + \frac{m}{ \phi^2 } + k ( \phi - 1 ) \), where \( n, l, m, k \) are integers ( \( l \geq 0 \), \( m = -l \dots l \), \( k \) can be negative). This form allows fractional adjustments while preserving the Fibonacci relation \( \phi^2 = \phi + 1 \), enabling closed-form solutions. For simplicity, we fit observed masses to simple expressions like \( p \phi^q \) (with \( p \) small integer, \( q = k \) or fractional via \( l/m \)), assigning quantum numbers to match (e.g., for pion, \( n=0 \), \( l=1 \), \( m=0 \), \( k=0 \), yielding \( n_\text{eff} = 1/\phi \)).
To arrive at correlations:
- Compute \( n_\text{eff} = 4 \times (m_\text{meas} / m_p) \).
- Find nearest integer \( n \) or fractional form using \( \phi \) powers/sums to minimize error ≤5%.
- Assign quantum numbers \( n, l, m, k \) to reproduce the form.
- Compute \( m_\text{comp} = (n_\text{eff} / 4) \times m_p \).
- Verify error and justify with broadening for resonances.
This was checked against PDG 2024 data for additional baryons, mesons, and interdisciplinary (leptons, quarks). Only new matches/near-matches within 5% are added, focusing on those requiring fractional \( \phi \)-based extensions. Quantum numbers now include S (strangeness), C (charm), B (bottomness), plus the new \( l, m, k \) (with base \( n \) often integer or zero for fractions).
Table of Correlations (Extended with New Entries)
Correlation Name | Quantum Numbers (J^P, I, S, C, B; n, l, m, k) | Computed Value (MeV) | Measured Value (MeV) | % Error | Justification (n_eff) | Comments |
---|---|---|---|---|---|---|
Proton | 1/2+, 1/2, 0, 0, 0; 4, 0, 0, 0 | 938.27 | 938.27 | 0.00 | n=4 | Exact match; base of PSM. |
Delta(1232) | 3/2+, 3/2, 0, 0, 0; 5, 0, 0, 0 | 1172.84 | 1232 | 4.80 | n=5 | Near match; resonance width ~100 MeV allows broadening. pp resonance correlation. |
N(1440) | 1/2+, 1/2, 0, 0, 0; 6, 0, 0, 0 | 1407.41 | 1440 | 2.26 | n=6 | Good match; Roper resonance, possible mixing. |
Delta(1600) | 3/2+, 3/2, 0, 0, 0; 7, 0, 0, 0 | 1641.48 | 1600 | 2.59 | n=7 | Match within error; broad resonance (Γ~300 MeV). |
N(1650) | 1/2-, 1/2, 0, 0, 0; 7, 0, 0, 0 | 1641.48 | 1650 | 0.52 | n=7 | Excellent match; negative parity excitation. |
N(1675) | 5/2-, 1/2, 0, 0, 0; 7, 0, 0, 0 | 1641.48 | 1675 | 2.03 | n=7 | Match; higher spin, modulation broadening. |
N(1680) | 5/2+, 1/2, 0, 0, 0; 7, 0, 0, 0 | 1641.48 | 1680 | 2.32 | n=7 | Match; close to N(1675), possible overlap. |
Delta(1700) | 3/2-, 3/2, 0, 0, 0; 7, 0, 0, 0 | 1641.48 | 1700 | 3.47 | n=7 | Match; Delta excitation, pp correlation. |
N(1710) | 1/2+, 1/2, 0, 0, 0; 7, 0, 0, 0 | 1641.48 | 1710 | 4.04 | n=7 | Near match; broadening due to decay modes. |
N(1720) | 3/2+, 1/2, 0, 0, 0; 7, 0, 0, 0 | 1641.48 | 1720 | 4.59 | n=7 | Near 5%; resonance with Γ~200 MeV. |
Delta(1900) | 1/2-, 3/2, 0, 0, 0; 8, 0, 0, 0 | 1876.54 | 1900 | 1.29 | n=8 | Good match; higher Delta state. |
Delta(1905) | 5/2+, 3/2, 0, 0, 0; 8, 0, 0, 0 | 1876.54 | 1905 | 1.55 | n=8 | Match; well-established. |
Delta(1910) | 1/2+, 3/2, 0, 0, 0; 8, 0, 0, 0 | 1876.54 | 1910 | 1.81 | n=8 | Match; clustering near n=8. |
Delta(1920) | 3/2+, 3/2, 0, 0, 0; 8, 0, 0, 0 | 1876.54 | 1920 | 2.34 | n=8 | Match; broad spectrum. |
Delta(1930) | 5/2-, 3/2, 0, 0, 0; 8, 0, 0, 0 | 1876.54 | 1930 | 2.87 | n=8 | Match; negative parity. |
Delta(1950) | 7/2-, 3/2, 0, 0, 0; 8, 0, 0, 0 | 1876.54 | 1950 | 3.94 | n=8 | Near match; high spin, modulation. |
Sigma(1193) | 1/2+, 1, -1, 0, 0; 5, 0, 0, 0 | 1172.84 | 1193 | 1.71 | n=5 | Match; strange baryon ground state. |
Omega(1672) | 3/2+, 0, -3, 0, 0; 7, 0, 0, 0 | 1641.48 | 1672 | 1.83 | n=7 | Match; hyperon, S=-3. |
D meson | 0-, 1/2, 0, 1, 0; 8, 0, 0, 0 | 1876.54 | 1867 | 0.51 | n=8 | Excellent match; charmed meson boson correlation. |
W boson | 1-, 1, 0, 0, 0; 343, 0, 0, 0 | 80430.32 | 80377 | 0.07 | n=343 | Very close; weak boson, large n correlation. |
Z boson | 1-, 0, 0, 0, 0; 389, 0, 0, 0 | 91249.95 | 91188 | 0.07 | n=389 | Very close; neutral weak boson. |
Higgs | 0+, ?, 0, 0, 0; 534, 0, 0, 0 | 125265.32 | 125250 | 0.01 | n=534 | Extremely close; scalar boson. (Alternate n=533 gives 0.18% error using PDG mass.) |
Top Quark | 1/2, ?, 0, 0, 0; 736, 0, 0, 0 | 172642.05 | 172690 | 0.03 | n=736 | Very close; heaviest quark, fermion correlation. |
Pion | 0^-, 1, 0, 0, 0; 0, 1, 0, -1 | 144.96 | 139.57 | 3.86 | n_eff = 1 / \phi | Light pseudoscalar meson; fractional golden quantum for quark-antiquark pair, interdisciplinary to meson sector. Broadening from pion cloud effects. |
Eta | 0^-+, 0, 0, 0, 0; 1, 1, 0, 0 | 524.5 | 547.86 | 4.27 | n_eff = \phi + 1 / \phi | Match with sum of golden powers; reflects flavor mixing (u,d,s), quasicrystal-like symmetry. |
Rho | 1^--, 1, 0, 0, 0; 2, 0, 0, 1 | 759.0 | 775.26 | 2.10 | n_eff = 2 \phi | Vector meson; golden extension for excited state, modulation in vector dominance model. |
Lambda(1116) | 1/2+, 0, -1, 0, 0; 5, 0, 0, 0 | 1172.84 | 1116 | 4.92 | n=5 | Good match; hyperon ground state, strangeness broadening. |
J/psi | 1^--, 0, 0, 0, 0; 13, 0, 0, 0 | 3050.39 | 3096.9 | 1.53 | n=13 | Charmonium state; bound cc-bar, effective large n from heavy quark. |
Upsilon(1S) | 1^--, 0, 0, 0, 0; 40, 0, 0, 0 | 9382.72 | 9460.3 | 0.82 | n=40 | Bottomonium state; bb-bar correlation, similar to J/psi but heavier. |
Tau Lepton | 1/2^-, 1/2, 0, 0, 0; 3, 0, 0, 2 | 1841.2 | 1776.86 | 3.62 | n_eff = 3 \phi^2 | Interdisciplinary to leptons; golden power fits heavy lepton mass, possible universal superfluid analogy. |
Lambda_c(2286) | 1/2+, 0, 0, 1, 0; 10, 0, 0, 0 | 2345.68 | 2286 | 2.55 | n=10 | Charmed hyperon; match with charm quantum, broadening from decay width ~0.2 MeV. |
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