Nuclear physics
The nucleus as a depth of persistence
PT treats the nuclear domain as an observation layer of the same structure: the channels that give Standard Model constants recombine into nuclear force, closures and binding energies.
The nuclear sector matters because it tests PT far away from its entry point: if the same cascade also explains nuclei, the theory gains considerable explanatory depth.
Same logic, deeper layer
The nucleus is read as a deeper persistence layer: colour, pions, closures and binding follow the same cascade.
Magic numbers
Without spin-orbit the model recovers 2, 8, 20; with the nuclear PT spin-orbit term it gives 2, 8, 20, 28, 50, 82, 126.
408/413 tests
The reported score is 408 passing tests out of 413, i.e. 98.8%, with zero fitted parameters.
L1
The nucleus is a deeper chemistry
One can enter nuclear physics without starting from equations. An atom has two layers of organization: outside, electrons make ordinary chemistry; at the centre, protons and neutrons make a much more compact, deeper chemistry, where the strong force replaces electromagnetism as the dominant channel.
PT therefore does not treat the nucleus as a separate continent. It asks a simple question: if persistence already organizes electrons, quarks, and colour channels, what does the same logic become when the degrees of freedom are trapped in a tiny, very dense volume?
The intuitive answer is shells. In an atom, closed electronic shells give noble gases. In a nucleus, proton and neutron shells can close too: these are the magic numbers. A nucleus near such a closure resists deformation better, binds more cleanly, and even changes its radioactive behaviour.
The central idea is this: nuclear stability is not just “a lot of strong force”. It is a geometry of channels. Some positions are exposed, others protected; some configurations close a shell, others leave a fragile boundary. PT tries to read that architecture with the same vocabulary as chemistry: channels, closures, depth, and echoes.
So the picture to keep is this: the nucleus is a very tight shell object. When a shell closes, the whole object becomes more stable; when it stays open, it becomes more reactive, more deformable, or more likely to decay.
- Protons and neutrons are the objects organized into shells.
- Nuclear closures are the deep analogue of noble gases.
- The strong force makes nuclear spin-orbit much more powerful than atomic spin-orbit.
- Radioactivity also depends on this architecture: a closure can suppress alpha preformation.
L2
How PT computes the nuclear sector
The monograph organizes the sector into eight families: equations, nucleon-nucleon potential, binding energies, magic numbers, radioactivity, reactions, NLO phases, and ab initio calculations.
The computation starts from constants already present in the theory: $s=1/2$, $N_c=3$, $C_F=4/3$ and the effective strong coupling. From there, PT reconstructs a nuclear potential, then the binding terms: volume, surface, Coulomb, asymmetry, pairing and closure corrections.
The important point is that these are not knobs adjusted to rescue a curve. The terms are continuous readings or shell corrections imposed by the PT hierarchy. That is precisely why the nuclear sector matters for a physicist.
- Potential: the colour channel leaves an effective residual between nucleons.
- Binding: Bethe-Weizsäcker-type mass formula, but with a PT dictionary.
- Shells: magic closures appear when internal channels close.
- Radioactivity: the factor $(5/8)^{n_{magic}}$ suppresses preformation near closures.
Magic numbers
Where do magic numbers come from?
In the usual nuclear shell model, magic numbers are often presented as the result of a mean potential plus strong spin-orbit coupling. The PT reading keeps that structure, but gives it a reason: nuclear depth amplifies spin-orbit because the strong channel replaces the electromagnetic scale.
At the discrete level, sieve depth $D=2$ gives four quantum numbers $(n,l,m_l,m_s)$. Without spin-orbit, the first closures 2, 8 and 20 are recovered, but the large nuclear closures are not forced.
With PT spin-orbit, the effective strength is $\lambda_{LS}=C_F\alpha_{s,eff}(\hbar c/(2m_\pi))^2\simeq0.475\,\mathrm{fm}^2$. Since $\alpha_{s,eff}/\alpha_{EM}$ is of order 100, the nucleus sees a much stronger spin-orbit splitting than the atom.
This is where the module becomes useful: the same channel logic explains why 28, 50, 82 and 126 appear. The closures correspond to the $0f_{7/2}$, $0g_{9/2}$, $0h_{11/2}$ and $0i_{13/2}$ orbitals dropping and opening the large gaps.
Nuclear shell closures
Without spin-orbit, the structure is too poor. With the nuclear spin-orbit term derived by PT, the seven standard closures are reconstructed.
L3
Technical demonstration: cascade, magic numbers, limits
The nuclear chapter belongs to physical validation: outputs are compared with experiment and structural tests. Its status is not that of a pure arithmetic identity such as GFT or T5, but of a derived cascade whose consequences are confronted with data.
The 5 failures are explicitly listed as limitations of the monopole approximation or three-body corrections, not as refutations of the cascade.
The technical cascade is $s=1/2\to N_c\to C_F\to\alpha_s\to\sigma_{QCD}\to f_\pi,m_\pi,M_N\to V_{NN}\to E_{bind}$. Each stage inherits constants already derived in earlier chapters.
For magic numbers, the route is explicit: $D=2$ gives $(n,l,m_l,m_s)$, the PT Woods-Saxon potential fixes the mean spectrum, then the derived LS term opens the 28, 50, 82 and 126 gaps. The responsible orbitals are $0s_{1/2}$, $0p_{3/2}$, $0d_{3/2}$, $0f_{7/2}$, $0g_{9/2}$, $0h_{11/2}$ and $0i_{13/2}$.
The 408/413 score mixes algebraic, structural, and empirical tests; the monograph indicates roughly 132 genuinely experimental comparisons. This is a major coherence test, but not 413 independent constants.
- $V_{NN}$ potential: OPE, $\sigma$, $\omega$, tensor components.
- Binding: Bethe-Weizsäcker + PT corrections, saturation near iron.
- Magic numbers: $2,8,20,28,50,82,126$ obtained with strong spin-orbit amplification.
- Radioactivity: alpha NLO with spectroscopic factor $(5/8)^{n_{magic}}$.
- Open: deuteron radius by tensor force, deformed nuclei, EOS beyond $2n_0$.
Echo of a magic closure
The spectroscopic factor used in alpha radioactivity is $(5/8)^{n_{magic}}$. Near a closure the shell echo is strong; far from it the effect fades continuously.
1.0
0.51
0.79
Près d’une fermeture, la préformation alpha est freinée.
Technical demonstration of the nuclear cascade
- The chain starts from constants already derived in the SM sector: $s=1/2$, $\mu^*=15$, $N_c=3$, $C_F=4/3$, $\alpha_{EM}$, and $\alpha_s$. Nuclear physics adds no continuous fitted parameter.
- The colour channel fixes the strong residual. The scales $f_\pi$, $m_\pi$, and $M_N$ inherit from the previous hadronic chain; they feed the nucleon-nucleon potential.
- $V_{NN}$ is decomposed into pion, sigma, omega, and tensor-like components. Each component corresponds to a different PT reading of colour residual and channel depth.
- Binding energies are then read through a Bethe-Weizsäcker-type mass formula with PT corrections: volume, surface, Coulomb, asymmetry, pairing, and closure corrections.
- Magic numbers are not pasted as a table: $D=2$ supplies the four quantum numbers, the PT Woods-Saxon potential gives the mean spectrum, then $\lambda_{LS}=C_F\alpha_{s,eff}(\hbar c/(2m_\pi))^2$ creates the large spin-orbit gaps.
- Alpha radioactivity is demonstrated through Gamow + PT corrections. The spectroscopic factor $(5/8)^{n_{magic}}$ reduces preformation near magic closures and replaces part of the full many-body solver.
- The reported 408/413 validation tests this cascade across eight families: equations, $V_{NN}$, binding, magic numbers, radioactivity, reactions, NLO phases, ab initio.
The PT reading of nuclear physics rests on a derived and validated cascade: SM-sector constants, colour residual, $V_{NN}$ potential, binding, magic numbers, and radioactivity. Its strength is coherence without continuous fitted parameters across many families, with known limits explicitly stated.
Sources monographie
- ch. 22d: Nuclear Physics, status box and ledger.
- pt_chimie_scores.tex: 408/413 tests, 98.8%.
- ch. 24: nuclear sector in post-programme directions.
- Appendix F: companion scripts and coverage.