WSM CORE CORPUS · PAGE 8 · HADRONS · 11 September 2026
PROTON, NEUTRON AND HIGHER STANDING-WAVE MATTER
Three precursor phase roles; one fused, continually rebuilt proton wave
Physical foundation
WSM Postulates
Open the postulates, units and frequency conventions
The complete WSM Action and its stable matter solution remain open. Explicit action candidates and exact reduced controls are displayed below. The A/B/C/D/Q tiers distinguish established relations, fixed WSM structure, concrete mechanisms, open calculations and excluded shortcuts throughout the page.
Units. \(c_0=E_{d0}=\lambda_0=1\). Hence \(f_0=1\) and \(\omega_0=k_0=2\pi\). The constants \(\hbar,m_e,\alpha,G\) are outputs, not units.
P1. One Substance. Space is a nearly rigid, slightly elastic wave medium whose only primitive motions are longitudinal plane waves propagating in all directions.
P2. One Law. Directional wave speed is determined by directional wave-energy density. For every direction \(\hat{\mathbf n}\),
Thus, in normalized units,
The universal intrinsic frequency \(f_0\) supplies the reference standard. Wavelength is the simultaneous crest spacing: speed and crest frequency in \(\lambda^{\prime}=c^{\prime}/f_{\rm crest}\) must use the same coordinates. Thus \(\lambda^{\prime}=c^{\prime}/f_0\) applies where \(f_{\rm crest}=f_0\). The intrinsic reference, fixed-position crest frequency and phase rate along a moving centre remain distinct readings.
P3. One Matter. Electron and positron are e-sphere wave centres formed from Huygens-combined longitudinal plane waves from all directions, with opposite background-relative radial phases. The e-sphere circumscribes a cube of side \(\lambda_0\):
Immediate deduction from P1. As the one substance, Space cannot be bounded, created or interrupted by another substance; it is therefore infinite, eternal and continuous.
P1–P3 are the fundamental postulates; additional working assumptions and approximations are stated where used. WSM Action must derive the complete spherical standing-wave and spherical phase-wave structure, their stability and all further physics.
WSM Wave Action: the mathematics already in hand
Open the Action equations and their present scope
An action turns a physical account into equations of motion. The WSM corpus already contains explicit action candidates, exact reduced dynamics and propagation controls. They establish concrete results and identify the coupling still needed for a stable, interacting e-sphere. The general variational form is
Here \(\mathcal C\) collects the independent variables describing longitudinal motion of the same Space. This schematic expression states the mathematical task; the following equations are actual constructions developed in the corpus.
Four constructions, four roles. \(S_0\) is the directional cycle-energy candidate; \(S_{\rm ray}\) supplies exact reduced ray dynamics; \(S_{\rm sphere}\) describes longitudinal spherical motion; \(S_{\rm control}\) isolates propagation through a prescribed profile. Their derivation as mutually consistent limits of one autonomous action remains to be established. An incompatibility between candidate pieces would reject that combination; it would not by itself refute P1–P3.
Directional cycle-energy action
Let \(C_{\hat n}(\mathbf x,t)\) describe the real longitudinal compression component travelling in direction \(\hat n\), and \(D_{\hat n}=\hat n\cdot\nabla\). The candidate defines the positive intensity ratio
where \(Q_{\hat n}\) and \(P_{\hat n}\) are cosine and sine projections of that compression over one reference cycle; the subscript 0 denotes the background. Its action is
With intensity held fixed, the characteristic speed is exactly \(c'_{\hat n}=c_0 I_{\hat n}\), recovering P2 from the kinetic and spatial coefficients. The full variation must also include the dependence of \(I\) on the wave history and constrain all directions to one physical displacement. A causal treatment of that history remains part of the construction. \(\chi_0\) is a declared normalization coefficient.
Exact dynamics in a one-dimensional ray model
For a compression coordinate \(q(\sigma,t)\), normalized strain \(a=q_\sigma/\epsilon_*\), and canonical imbalance \(\eta\), the corpus gives
Variation yields two oppositely travelling characteristic families. Their positive energy responses and speed magnitudes satisfy \(E_\pm/E_{d0}=c_\pm/c_0=e^{a\pm\eta}\). Choosing \(\eta=\operatorname{artanh}\beta\), \(a=\tfrac12\ln(1-\beta^2)\), and \(\beta=v/c_0\) gives \(e^{a\pm\eta}=1\pm\beta\); removing the common geometric mean gives \(e^{\pm\eta}=\gamma(1\pm\beta)\), where \(\gamma=(1-\beta^2)^{-1/2}\). These are exact results within this ray model. Its uncoupled local transport does not generate the spherical core from a homogeneous background.
Longitudinal spherical action
Writing displacement as \(\mathbf u=\nabla\Psi\) gives a reduced action with positive coefficients \(\rho_\Psi\) and \(\kappa\):
The unforced equation admits the regular spherical \(j_0\) compression mode and its quarter-cycle \(j_1\) radial motion. The source term \(f_\Psi\) currently stands for the incoming Huygens relation. Deriving that relation from the surrounding matter is the step needed to make the recurrence self-consistent.
An exact propagation control
For a prescribed positive, stationary profile \(\epsilon(x)\), the action displayed on the homepage is
The coordinate \(y=\int dx/\epsilon(x)\) converts it to a uniform wave action. In this prescribed, stationary one-dimensional profile, a complete transmitted pulse is reflectionless and gives zero net impulse on the profile when the response is the same at both ends. Local force density need not vanish: its contributions cancel in the total impulse. A changed travel time alone therefore does not establish a net force. This control contains no receiving e-sphere and does not calculate its gravitational response. The prescribed profile is an input to this control.
The next calculation is specific. Join the directional response, longitudinal displacement and continuing Huygens waves through one independent state and one energy–momentum account. Then solve an open periodic e-sphere at P3’s fixed \(R/\lambda_0=\sqrt3/2\), with finite excess energy and a complete stability spectrum. The existing actions and exact controls supply mathematical starting points; a complete self-consistent WSM Action and its stable matter solution remain to be obtained.
Equations and their assumptions: WSM Action, §13: present mathematical pieces; §14: the open boundary problem; and homepage Action summary and propagation control.
Can the same real longitudinal waves and finite e-sphere geometry fixed for the electron reclose as a stable proton—one inseparable three-role wave whose mass, charge, spin, persistence, radii, magnetic moment, neutron relation and QCD scattering response all come from one unchanged Action of vibrating Space?
Abstract
Scientific collaboration question. Can three precursor e-sphere phase roles fuse into one stable proton recurrence whose complete response reproduces proton, neutron and QCD observables?
Working hypothesis. A hadron is a nonlinear relative-periodic standing-wave organisation of the same vibrating Space—not permanent particles held by a second substance.
Foundation. One substance: Vibrating Space — One law: c′/c0 = Ed/Ed0.
Reading direction. Follow the incoming waves through fusion. Keep formation history distinct from finished ontology. Demand one solution for every read.
Use the shared claim-status key for the labels throughout this essay.
Picture the formation before naming its algebra. Three open e-spheres approach through one already vibrating Space. Each is an all-direction relation: longitudinal plane waves converge from its Huygens domain, flow through its finite core and continue outward. Their extended wave eggs overlap before any wave centre meets another. The waves do not collide like hard beads. Direction by direction, compression and extension superpose; directional \(E_d\) changes; by the One Law \(c'\) changes; and wavelength, phase, wavefront curve, convergence and centre reconstruction change with it.
If the encounter disperses, three independent recurrences leave. If it captures, their old phase closures cannot simply remain side by side. Changed out-waves from each centre cross fresh waves travelling toward the others. Those crossings alter the in-wave geometry that reaches the next recurrence. The process cascades until either excess relative energy escapes on continuing waves or no stable closure exists. The proton hypothesis is the successful branch: the three precursor centres lose independent identity and one compact relative-periodic wave closes. Its three phase roles remain as an internal mode basis, not as three little particles orbiting inside a shell.
Current answer
Formation history is not finished ontology.
The \(++-\) ancestry gives a minimal signed formation ledger and concrete kinematic controls. It does not license additive lobe masses, permanent internal muons or three fitted orbit speeds. In the finished proton there is one relative energy, one centre, one conserved current and one Floquet spectrum.
Claim-status key
Claim-status key
| Tier | Meaning |
|---|---|
| A | Established experiment, standard result or exact mathematics under explicitly stated premises. |
| B | Fixed WSM postulate or direct deduction from the real-wave ontology and established geometry. |
| C | Concrete physical construction whose decisive calculation or test is specified. |
| D | Required quantitative output of WSM Action. |
| Q | Rejected route or ontology error retained only in the failure ledger so it is not repeated. |
Essential WSM glossary
Open the essential WSM terms
From a metaphysics of Space and Time to a metaphysics of Space and Motion.
Newtonian mechanics describes matter particles moving in space and time, with mass and force entering its laws of motion. Its gravitational law gives attraction between separated bodies without specifying a local transmitting mechanism. WSM applies motion directly to Space: the wave motion of one continuous physical substance forms matter, and its ordered change supplies what clocks measure as time. Matter and time are understood through the activity of Space itself.
Newton himself objected to unmediated action at a distance: his letter to Richard Bentley distinguishes the law of attraction from its physical cause.
| Term | Meaning in WSM |
|---|---|
| Vibrating Space | One infinite, eternal, continuous, nearly rigid, slightly elastic wave medium. This physical substance supports longitudinal compression plane waves whose organisation forms matter. Time measures its ordered wave change. |
| Background wave sea | The longitudinal compression plane waves travelling through Vibrating Space in all directions. |
| Directional wave-energy density \(E_d\) | Wave-energy density associated with a specified direction of propagation. \(E_{d0}\) denotes its background value. |
| Physical wave speed \(c'\) | The local propagation speed of a longitudinal plane wave in a specified direction. \(c_0\) denotes the background reference speed. |
| Spherical standing wave | Formed by the coherent Huygens combination of incoming longitudinal plane waves from all directions. The waves cross the centre and continue outward. The finite central core of high directional wave-energy density \(E_d\) is called the e-sphere. WSM identifies its two opposite radial phases relative to the vibrating background as the electron and positron: a matter–antimatter pair. |
| Huygens sphere | The finite all-direction wave relation through which surrounding matter supplies an e-sphere’s incoming waves. |
| Reconstruction / reclosure | Reconstruction is the repeated formation of an e-sphere by waves passing through it. Reclosure is the restoration of its complete phase relation. |
| Curve on a plane wave | The half-spherical displacement and phase profile imprinted on a passing plane wave as it crosses an e-sphere. |
| Curve train | A finite, ordered sequence of changed curves written onto passing background waves during a bound-state transition. This is WSM’s description of a photon. |
| Moving wave egg | The asymmetric wave organisation of a moving e-sphere, with an elongated front and flattened rear. |
| Spherical phase wave | The moving pattern of equal-phase positions formed by intersecting longitudinal waves across an e-sphere. Its two opposite directions of phase rotation are called its two “hands”. |
| Huygens ring | The circle of contributing longitudinal-wave directions perpendicular to a light train’s direction of propagation. |
| Phase-even residual delay | The component of wave delay unchanged by reversing the radial phase. This is the residual used in WSM’s gravity account. |
| WSM Action | The programme for expressing the dynamics of WSM’s single wave medium through an action whose variation gives the equations of motion. |
Extended WSM reference: the complete glossary, definitions and research notes.
Part I — Foundation and Physical Formation
1. P1–P3 and the one causal chain
P1 · One Substance Space is a nearly rigid, slightly elastic wave medium whose primitive motions are real longitudinal compression and extension plane waves propagating in all directions.
P2 · One Law For every direction \(\widehat{\mathbf n}\),
Directional wave-energy density changes the local longitudinal-wave speed in that direction. A complete interaction therefore changes travel time, wavelength, phase and wavefront geometry together.
P3 · Matter Geometry Electron and positron are finite e-sphere wave centres formed from Huygens-combined longitudinal plane waves arriving from all directions, with opposite background-relative radial phases. The e-sphere circumscribes a cube of side \(\lambda_0\), so \(R=\sqrt3\lambda_0/2\).
Everything on this page follows that chain. No binding field is added between independently existing particles. If a proton exists in WSM, its binding is the self-consistent recurrence of the same Space whose waves constitute the precursor e-spheres.
2. Real-wave vocabulary: what each word points to
| Term | Real wave meaning | Do not turn it into |
|---|---|---|
| e-sphere | a finite core and extended all-direction in-wave/out-wave relation reconstructed continuously | a rigid spherical membrane |
| wave egg | the direction-dependent \(E_d,c'\), wavelength, phase, curve and convergence of a moving or interacting recurrence | a material shell being mechanically squeezed |
| precursor role | a radial-phase and spherical-hand relation that helped form the fused recurrence and remains as a delocalised mode coordinate | a permanent muon pellet |
| centre | the recurrent intersection reconstructed by the complete arriving phase sky | a primitive point substance |
| binding | one lower-relative-energy phase closure maintained by real waves flowing through it | a second invisible glue |
| radiation | the non-recurrent difference carried away on continuing waves during capture or transition | loss of the persistent balanced in/out recurrence itself |
| threefold role | a \(C_3\)-capable basis within one nonlinear field history | QCD colour already derived |
The language “three e-spheres form a proton” describes a candidate history. Once fusion succeeds, the cleaner sentence is: one proton wave carries three coordinated precursor-phase roles.
3. Capture as a living wave-feedback cascade
C · physical construction The fusion is not a single collision event. It is a delayed, many-pass reorganisation of real waves:
- Two positive-phase and one negative-phase muonic-scale e-spheres enter with a closed total momentum triangle. Their extended wave relations already overlap.
- Where their longitudinal waves cross, the relative phases change the complete directional \(E_d\). The One Law changes \(c'\) on those portions of the plane-wave fronts.
- Changed travel times bow and shear the wavefront pattern. The three wave eggs deform; their reconstructed centres shift; their spherical phase hands torque and precess.
- Those newly changed waves do not return. They continue outward. On the way they cross other waves already travelling inward toward all three centres and write new timing and curvature onto them.
- The newly conditioned in-waves reach the interaction region and rebuild the next state. Thus each e-sphere receives a delayed physical consequence of the changed waves emitted during the preceding pass.
- Unmatched phase and excess relative energy leave in radiative trains. Matched relations reinforce a common recurrence.
- If a stable branch exists, the three former centres cease to reclose independently. One centre and one relative-periodic three-role wave remain.
That cascade is the visual content behind the nonlinear solver. A converged proton is the fixed or relative-periodic orbit of the map; an unstable candidate amplifies a sideband, splits or radiates away.
Part II — Formation Controls and Fused Geometry
4. The exact three-precursor kinematic control
A · conditional arithmetic Start with the declared candidate channel
If three free on-shell muonic precursors share the proton rest energy equally, each carries
Three equal translational momentum vectors can close in one plane at \(120^\circ\):
The associated reciprocal Doppler ratio is
Use these numbers where they were derived.
\(\gamma_{\rm form}\), \(\beta_{\rm form}\), \(p_{\rm form}\) and \(33.02\) describe an equal-energy incoming control built from measured proton and muon masses. They do not become permanent internal velocities by relabelling. In the fused solution an energy-role ratio is not a local speed unless the reconstructed displacement history supplies one.
5. Three is the MDL-leading branch, not a hidden theorem
One extra positive precursor gives
Under the same equal-energy free-muon control,
| \(N\) | Signed ancestry | \(\gamma_N\) | \(\beta_N\) | Blind-control reading |
|---|---|---|---|---|
| 1 | \(1+,0-\) | 8.880 | 0.9936 | one lepton-like ancestry; no composite three-role seed |
| 3 | \(2+,1-\) | 2.960 | 0.9412 | smallest composite candidate |
| 5 | \(3+,2-\) | 1.776 | 0.8264 | kinematically allowed competitor |
| 7 | \(4+,3-\) | 1.269 | 0.6153 | kinematically allowed competitor |
| \(\ge9\) | odd family | \(<1\) | — | excluded by this particular free on-shell equal-energy premise |
C · selection hypothesis \(N=3\) is the minimum-description-length starting branch because it is the smallest composite ancestry with net \(+e\), odd lifted parity and a three-sector mode basis. The solver must still admit \(N=5\) and \(N=7\) histories and discover whether only \(N=3\) falls into the stable proton attractor. Selection by stability is physics; selection by never testing the competitors is syntax.
6. The exact \(C_3\) basis belongs to one fused wave
The signed ancestry \((1,1,-1)\) is not itself an eigenvector of cyclic permutation. The exact cyclic basis is
A · origin-independent chiral dipole For role positions \(\mathbf x_j\), define
After translating every role by \(\mathbf a\),
The symmetric component may carry the net exterior signed response, while \(v_\pm\) carry neutral chiral circulation whose dipole cannot be erased by shifting the coordinate origin. These are delocalised normal coordinates of the complete proton displacement—not three separately locatable things.
C · relative-periodic use A successful proton may combine a spatial \(2\pi/3\) rotation with an internal radial-phase or spherical-hand operation. Instantaneous density need not be perfectly \(C_3\)-symmetric; the recurrence can restore the relation only after the combined operation.
7. Spin, exchange and the proton–Delta discriminator
B · odd lifted closure If each precursor mode already has the e-sphere's derived lifted sign, an odd locked ancestry retains
This does not identify electric sign with spin hand. Proton and antiproton each permit either measured spin projection; charge conjugation and reversal of spherical hand are separate operations.
The exact representation decomposition is
The two equal positive-phase roles can enter the \(J=\tfrac12\) sector through different exchange couplings, while an aligned \(J=\tfrac32\) sector is also available. The nonlinear recurrence must select the proton's \(J^P=\tfrac12^+\) ground branch and the complementary spatial–orientation symmetry required by exchange.
C · rotational-band control If the lowest aligned branch behaves like a collective rotor,
The measured proton–Delta spacing therefore gives an empirical inertia benchmark. A real success is one independently solved orientation band returning that spacing without fitting its inertia to the same measured separation while the one-e-sphere electron solution does not acquire an analogous low-lying \(J=\tfrac32\) partner.
8. Electric charge, spin lift and baryon persistence are different ledgers
A signed direction map on an enclosing \(S^2\) may carry an integer degree. That is a candidate route to indivisible electric response. It cannot also explain proton longevity, because the charge-preserving ancestry reversal
is open by approximately \(621.3\,{\rm MeV}\) in bare rest-energy arithmetic. The observed proton does not promptly fall apart. Its finished wave therefore needs a closure absent from both electric sign and the separated precursor state.
C · independent baryon candidate If a solved orientation variable approaches one value at spatial infinity, compactified physical space is \(S^3\). A quaternion orientation map \(Q:S^3_{\rm space}\to S^3_{\rm orientation}\) admits
This is a concrete persistence candidate for a fused three-dimensional recurrence. It remains separate from an electric \(S^2\) degree and from the \(4\pi\) spin lift. The action may instead supply a very high energetic or coherent-unwinding barrier, but one of those mechanisms must be visible in the solved decay spectrum.
9. One relative energy; one relative-periodic recurrence
Against the active background \(Z_{\rm sea}\), the proton energy must subtract both the background value and its tangent:
This keeps the living sea from being counted again as proton mass. Cross terms, gradients, phase currents, orientation stress and the open exterior all belong to the same energy ledger. Adding three isolated rest energies after fusion would discard the interaction that defines the new object.
The minimal three-dimensional recurrence target is
Here \(\mathcal R_{2\pi/3}\) rotates or permutes the spatial roles and \(\mathcal U\) performs the required internal phase/hand operation. The primitive temporal period is a blind output. A stationary proton is not a frozen lump and not “no out-wave”: real waves continually cross its centre and leave, while the completed orbit returns with zero mean excess four-momentum flux.
Linearise around the solved orbit. Its monodromy operator \(\mathcal M_p\) must have only the neutral multipliers required by exact symmetries; all other physical multipliers must lie on the stable unit circle with acceptable Krein signatures, while open-channel resonances obey outgoing radiation conditions.
Part III — Physical Reads and the Empirical Tribunal
10. One conserved current must produce moment, radii and form factors
The proton has no hard classical edge. Keep four scales distinct:
| Scale | Real-wave meaning | How it is read |
|---|---|---|
| \(R_{\rm mode}\) | where the compact recurrence carries substantial relative action | direct solver profile |
| \(R_{\rm phase}\) | where its phase and orientation reclose | phase-map diagnostic |
| \(r_E\) | electric response radius | \(r_E^2=-6G_E'(0)\) |
| \(r_M\) | magnetic response radius | \(r_M^2=-6G_M'(0)/G_M(0)\) |
The geometrical clue \(4\bar\lambda_\mu/9\approx0.830\,{\rm fm}\) is a C-level skeleton near the measured proton charge-radius scale. It is not the charge radius until the calculated current gives that form-factor slope.
The magnetic moment is the circulation read of the whole conserved current:
A · response target Conventional elastic scattering packages the measured current as
WSM must obtain these functions as projections of its one current. A long probe wave reads the coherent net exterior. A shorter probe arrives with phase variation across the compact recurrence and reads different correlations among the three delocalised roles. The returned angular residues describe how the whole wave answered; they do not by themselves prove pre-existing point constituents.
11. QCD is the quantitative tribunal, not a vocabulary to be replaced
Quantum chromodynamics successfully organises hadron symmetries, spectra, scaling violations, jets and strong-interaction amplitudes. WSM earns a deeper physical reading only by reproducing that structure from the same action that made the electron and proton. \(C_3\) is not \(SU(3)\); three precursor roles are not automatically three colours; response fractions are not automatically permanent fractional charges.
| QCD/experiment target | Real-wave question for the fused recurrence | Required output |
|---|---|---|
| confinement and absence of free colour | why does trying to isolate one short-distance response sector deform or destroy the whole recurrent mode? | rising separation energy or unavoidable reclosure into colour-neutral asymptotic waves |
| asymptotic freedom and running | does a shorter probe interact with progressively less of the coherent recurrence before nonlinear rebuilding occurs? | the measured beta function and scale dependence, not merely qualitative weakening |
| fractional response weights | how do \(C_3\) phase coordinates project onto the probe current? | correct charges, flavour weights and sum rules without inserting constituent fractions |
| deep-inelastic scaling violations | how does the finite wave distribute momentum among resolved modes and its radiative exterior? | positive PDFs/GPDs, evolution kernels and momentum/valence sum rules |
| jets and hadronisation | how does a violently opened coherent recurrence release narrow directional trains and then reclose them into stable matter waves? | multiplicity, angular, flavour and energy-systematics of observed jets |
| hadron spectrum | what other stable, metastable and resonant relative-periodic closures share the action? | quantum numbers, masses, widths and transition matrix elements |
| chiral and axial physics | how do opposite phase/hand sectors respond to handed probes? | \(g_A\), pion relations, weak currents and symmetry-breaking pattern |
| lattice-QCD results | can the WSM solver match nonperturbative masses, form factors and matrix elements? | agreement on observables from different numerical formulations |
Two compact benchmark equations keep the target sharp. At short distance, QCD requires the non-Abelian running
and the resolved momentum ledger obeys
The WSM scattering operator must recover their measured content in its effective coordinates while keeping the ontology one Space. A pretty three-lobed picture that misses these outputs fails.
12. The neutron is a neighbouring bifurcation, not a fourth stored lepton
A literal fourth independent spinorial lobe would give \((-1)^4=+1\) under a common \(2\pi\) turn, whereas the neutron is spin-\(\tfrac12\). The compact notation \(N=P[-]\) can therefore mean only a collective boundary or phase bifurcation of a \(B=1\) spinorial wave—not a proton holding an already closed electron inside it.
C · global transition Beta decay is
The changing neutron recurrence writes new outgoing wave relations that asymptotically close as a proton, electron and antineutrino. The electron need not have pre-existed as an independent electron core inside the neutron. The same action must calculate the neutron–proton mass difference, axial current, phase-space endpoint, transition overlap and lifetime.
13. Antiproton, neutral matter and the phase-even stress read
Reverse every radial-phase sign and the candidate becomes an antiproton recurrence. The charge-odd exterior reverses; the phase-even relative energy and stress do not. For the minimal neutral hydrogen ancestry,
For antihydrogen every \(s_i\) reverses, leaving the even sum and positive relative energy unchanged. This supplies a compact WSM reason that electric neutrality need not erase gravity and that matter and antimatter should share the same gravitational sign. The ALPHA-g antihydrogen result is consistent with attraction toward Earth. The magnitude and universality of gravity must come from the full phase-even stress response, not the bare count four.
14. Mesons, baryons and higher standing-wave matter
D · family search The proton proposal matters only if it opens a calculable family rather than an isolated story. Use the same frozen action and boundary sea to search:
| Family | Candidate real-wave organisation | Blind outputs |
|---|---|---|
| meson-like | opposite signed roles with no baryon winding, closing as a finite bosonic relative-periodic wave | spin/parity families, masses, widths, charge conjugation and decay channels |
| baryon-like | odd lifted fused recurrences in nonzero baryon sector | octet/decuplet-like organisation, excitations, moments and transitions |
| radial/orientation excitations | higher Floquet branches of one recurrence | resonance masses, widths and selection rules |
| multi-baryon | phase-locked relations among complete baryon recurrences | deuteron binding, nuclear forces and saturation without a new substance |
| opened high-energy state | temporarily deconfined response of a violently driven recurrence and sea | jet, multiplicity, thermal and recombination systematics |
Names such as “meson” and “baryon” refer here to empirical quantum-number families whose effective QCD description remains compulsory. The WSM task is to discover which recurrent geometries generate them and which candidate geometries do not survive.
Part IV — Calculation, Failure and Compression
15. Freeze one Action; solve one three-dimensional open recurrence
The hadron calculation is not a three-body orbit integration. It is an open-boundary nonlinear relative-periodic solve in the same canonical variables and normalisation already fixed by the electron/QED programme.
15.1 Inputs fixed before comparison
- P1–P3, the calm directional sea and one frozen WSM Action.
- The action's already-derived electron and positron branches, action scale, conserved current and two spherical hands.
- Total asymptotic charge \(+1\), candidate baryon sector \(B=1\), zero total momentum and the \(J^P=\tfrac12^+\) search sector.
- Open radiation conditions and tangent-subtracted relative energy.
- \(N=3,5,7\) precursor histories used only as initial basins, never as fitted final shapes.
- Numerical resolution, domain, continuation parameters, stability tolerance and observable projections registered before target comparison.
15.2 Sector checks and blind outputs from the unchanged solve
Charge, baryon sector and spin/parity specified in §15.1 are search conditions. The calculation must establish whether a stable solution exists with those properties; their specification is not itself a blind prediction. Mass, magnetic moment, form factors and further branches are independent prediction targets when calculated without fitting them to the corresponding measured values.
15.3 Physical convergence test
Increase the domain and angular/radial resolution. A genuine proton branch must retain its relative energy, current, low multipliers and form-factor slopes while outgoing transients move farther away. Numerical confinement by a box wall, imposed \(C_3\) symmetry or frozen precursor labels is not physical stability.
16. Direct failure conditions
| Read | Required result | Failure |
|---|---|---|
| ontology | one displacement/coherence state with representations constrained to it | independent binding or colour substance is inserted |
| existence | stable compact open recurrence | collapse, dispersion or box-supported pseudo-solution |
| selection | the proton branch wins without excluding competitors by hand | \(N=3\) is merely preloaded |
| mass | \(m_p\) from one relative action and existing calibration | new proton scale or additive precursor masses |
| spin | stable \(J^P=\tfrac12^+\), \(4\pi\) closure and correct excitation pattern | wrong parity, rigid body axis or unobserved low branches |
| charge | one conserved signed exterior with antiproton partner | leaking or continuously tunable net charge |
| persistence | independent winding or calculated suppression of open disassembly | prompt decay to the charge-preserving ancestry channel |
| size and moment | one current gives \(\mu_p,r_E,r_M\) and full form factors | separate fitted internal pictures |
| neutron/weak | mass splitting, axial response, beta spectrum and lifetime | stored-electron story or sector-specific weak rule |
| QCD | quantitative running, fractions, sum rules, colour algebra, spectra and jets | “three roles” replaces calculation |
17. Quarantine: preserve the lesson, remove the route
Permanent muons inside the proton
Retire. Muonic mass sets a candidate formation scale. A completed proton is one nonlinear recurrence, not three free muons stored inside it.
Additive lobe masses and fixed internal orbit speeds
Retire. The fused energy contains cross terms, gradients, phase currents and orientation stress. Formation \(\beta\) is not an internal speed.
Threefold geometry equals QCD colour
Retire as a derivation. \(C_3\) may seed three response coordinates; \(SU(3)\) algebra, colour factors, running and scattering must emerge quantitatively.
Electric charge also protects baryon number
Retire. \(p\to2\mu^++\mu^-\) preserves charge and is energetically open. Proton persistence needs a different relation.
Neutron as proton plus a stored electron
Retire. It gives the wrong simple spin-sign count and does not calculate beta decay. Seek a neighbouring whole-wave \(B=1\) bifurcation.
One guessed radius is every radius
Retire. Mode support, phase closure, electric slope and magnetic slope are distinct reads of one solved state.
18. Minimum-description-length synthesis
That is the promised compression. It is stronger than attaching a different picture to each observable because every read constrains the same recurrent displacement. It is also more vulnerable: one bad spin branch, one leaking current, one missing QCD factor or one unstable Floquet multiplier can reject the construction.
The physical picture remains alive. Real plane waves enter from all directions. They cross a compact recurrence and leave with changed phase and curvature. During formation, three extended e-sphere relations repeatedly alter one another's future in-waves. Excess mismatch flows away. A common three-role rhythm closes and is rebuilt at every cycle. Later probe waves do not strike hidden pellets; they deform that rhythm, and its entire current answers. The mathematics must become the faithful compression of this motion.
The proton page has one central demand: do not derive each proton fact separately. Make one wave and ask it every question.
19. Primary sources and WSM corpus handoff
19.1 Empirical and mathematical anchors
- Particle Data Group: current particle properties, baryon quantum numbers, masses, widths and review conventions.
- NIST/CODATA fundamental constants: proton and muon mass data and magnetic quantities used in the conditional formation controls.
- ALPHA Collaboration, observation of gravity's effect on antihydrogen.
- PDG 2026 review collection: QCD, quark model, structure functions, form factors and hadron spectroscopy.
19.2 WSM corpus handoff
- Action of Vibrating Space: P1–P3, the directional action problem, fixed e-sphere core, moving wave egg and solver gates.
- Mathematical Physics: the shared implication ledger, exact \(C_3\) controls, relative energy and hadron programme.
- Dirac and QED: the four e-sphere state coordinates, conserved current, source–receiver response and precision gates inherited by the hadron solve.
- Quantum Theory: discrete closure, measurement, many-body state construction and transition rules.
Geoffrey Haselhurst, in Human–AI scientific collaboration. Reconstructed in current WSM real-wave language, 11 September 2026.