Tuesday, July 8, 2025

Comparing Models to QCD and Accepted Values #2

Comparison of Proton Models Including QCD

Comparison of the Quantized Vortex Superfluid Proton Model, the 2-Bell Harmonic Analogy, and QCD

This document compares three theoretical approaches—the Quantized Vortex Superfluid Proton Model, the 2-Bell Harmonic Analogy, and Quantum Chromodynamics (QCD)—evaluating their predictions for the proton radius and correlations with proton resonances (e.g., Ξ” and N) and higher-order resonances (e.g., Higgs boson). It includes equations, tables with experimental values, errors, and scores to assess how well each model's predictions align with accepted data.

1. Introduction

The purpose of this comparison is to analyze the accuracy of each model in predicting key proton properties. The Quantized Vortex Superfluid Proton Model conceptualizes the proton as a quantized vortex in a superfluid medium, the 2-Bell Harmonic Analogy uses harmonic frequency differences to model particle energies and widths, and QCD, the fundamental theory of the strong force, describes quark and gluon interactions. Predictions are benchmarked against experimental measurements.

2. Model Descriptions

2.1 Quantized Vortex Superfluid Proton Model

This model represents the proton as a quantized vortex in a superfluid, with energy levels determined by a quantum number \( n \). The energy is calculated as:

\[ E_n = \frac{n}{4} \times 938.272 \, \text{MeV} \]

Here, \( 938.272 \, \text{MeV} \) is the proton rest mass energy, and \( n = 4 \) corresponds to the proton (\( E_4 = 938.272 \, \text{MeV} \)). Higher \( n \) values predict excited states or other particles, such as the Higgs boson at \( n = 533 \).

2.2 2-Bell Harmonic Analogy

This analogy models particle properties using two detuned frequencies, \( f_1 = 234.568 \, \text{Hz} \) and \( f_2 = 257.568 \, \text{Hz} \), where frequency (Hz) is analogous to energy (MeV). The average energy and width for harmonic \( n \) are:

\[ E_{\text{avg}, n} = n \times 246.068 \, \text{MeV} \] \[ \Gamma_n = n \times 23 \, \text{MeV} \]

These equations estimate the central energy and decay width of resonances.

2.3 Quantum Chromodynamics (QCD)

QCD is the established theory of the strong interaction, governing quarks and gluons. At low energies, relevant to proton structure and resonances, predictions rely on non-perturbative techniques like lattice QCD simulations due to the breakdown of perturbative methods.

  • Proton Radius: Lattice QCD predicts the proton charge radius as \( r_p = 0.831 \pm 0.010 \, \text{fm} \), aligning closely with the experimental value of \( 0.841 \, \text{fm} \).
  • Resonances: Lattice QCD estimates resonance masses (e.g., \( \Delta(1232) \) at \( 1210 \pm 50 \, \text{MeV} \)), though widths are harder to compute directly and may involve additional modeling.

3. Proton Radius Predictions

3.1 Quantized Vortex Model

The proton radius is derived from the vortex circulation, where the velocity at \( r_p \) equals the speed of light:

\[ r_p = \frac{n h}{2\pi m_p c} \]

For \( n = 4 \), this yields \( r_p \approx 0.840 \, \text{fm} \). A refined version using the fine-structure constant \( \alpha \), Rydberg constant \( R_\infty \), and hydrogen radius \( R_H \) is:

\[ \alpha^2 = \pi \cdot r_p \cdot R_\infty \cdot \frac{R_H}{R_\infty - R_H} \]

This also predicts \( r_p \approx 0.840 \, \text{fm} \), very near the experimental value.

3.2 2-Bell Analogy

The 2-Bell Harmonic Analogy does not offer a direct prediction for the proton radius.

3.3 QCD

Lattice QCD simulations compute the proton radius as \( r_p = 0.831 \pm 0.010 \, \text{fm} \), based on quark and gluon field configurations.

3.4 Comparison Table

Model Predicted \( r_p \) (fm) Experimental Value (fm) Error (%)
Quantized Vortex Model 0.840 0.841 0.12
2-Bell Analogy N/A 0.841 N/A
QCD (Lattice) 0.831 ± 0.010 0.841 1.19

The Quantized Vortex Model and QCD predict proton radii with errors of 0.12% and 1.19%, respectively, compared to the experimental \( 0.841 \, \text{fm} \). The 2-Bell Analogy does not address this property.

4. Resonance Correlations

This section evaluates predictions for the masses and widths of proton resonances and the Higgs boson. A correlation is assigned if the predicted mass is within 5% of the accepted value.

Resonance Accepted Mass (MeV) Accepted Width (MeV) Quantized Vortex \( E_n \) (MeV) 2-Bell \( E_{\text{avg}, n} \) (MeV) 2-Bell \( \Gamma_n \) (MeV) QCD Prediction (MeV) Correlation (Quantized Vortex) Correlation (2-Bell) Correlation (QCD)
Proton (\( n = 4 \)) 938.272 0 938.272 984.272 92 938.272 (exact) Yes No Yes
\( \Delta(1232) \) (\( n = 5 \)) 1232 115 1172.84 1230.34 115 1210 ± 50 No Yes Yes
\( N(1440) \) (\( n = 6 \)) 1440 300 1407.408 1476.408 138 1420 ± 60 Yes Yes Yes
\( N(1710) \) (\( n = 7 \)) 1710 100–200 1641.976 1722.476 161 1680 ± 70 Yes Yes Yes
\( \Delta(1950) \) (\( n = 8 \)) 1950 235 1876.544 1968.544 184 1920 ± 80 Yes Yes Yes
\( N(2220) \) (\( n = 9 \)) 2220 400 2111.112 2214.612 207 2200 ± 90 Yes Yes Yes
Higgs Boson (\( n = 533 \)) 125,000 4.07 125,000 N/A N/A 125,000 (SM) Yes No Yes

Notes: QCD resonance predictions are approximate, derived from lattice QCD or effective models. The Higgs boson mass is a Standard Model prediction, not directly from QCD alone.

4.1 Correlation Scores

The table below summarizes the number of resonances with predicted masses within 5% of accepted values.

Model Number of Correlations
Quantized Vortex Model 6
2-Bell Analogy 5
QCD 7

QCD scores highest with 7 correlations, reflecting its accuracy for the proton, key resonances, and the Higgs boson (via the Standard Model). The Quantized Vortex Model follows with 6, excelling for the proton and Higgs, while the 2-Bell Analogy achieves 5, with strong resonance matches but limited scope.

5. Conclusion

The Quantized Vortex Model and 2-Bell Analogy provide innovative phenomenological approaches with impressive correlations to experimental data. However, QCD, as the fundamental theory, offers the most robust and comprehensive predictions, despite relying on complex simulations for low-energy properties. Its superior score underscores its foundational role in particle physics.

6. References

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