Conditional GeV values · one electron anchor
Three compiled free masses, with one empirical anchor
Finite detector · conditional calibrated source
A mass readout with finite exposure
A 32-outcome pointer measures energy evolution without first reading an exact family label. An exactly equivalent adaptive implementation uses one reusable quantum qubit, five retained bits and five sequential source services. All 8,010 probe/detector records survive. Ideal coverage is at least 65/72 for normalized one-excitation inputs at the phase detector. On the full post-probe source, bad-phase-record probability is bounded by 7/72 times the original one-excitation weight. Vacuum and many-excitation records remain terminal without a mass interval; hardware precision and calibration errors are separate.
All 32 phase outcomes for this source energy
The displayed kernel is the complete pointer law for a declared energy input. The linked receipt retains every original probe weight, vacuum and many-excitation complement.
| Pointer bin | Probability | Ideal mass confidence set (GeV, rounded) |
|---|
Calibrated neutrino inputs · Majorana phase remains free
Neutrino masses and a complete phase envelope
These are consequences of the supplied mass and mixing packet, not independent predictions. The neutral contraction retains six success outcomes, failure and the full spectator complement, and preserves references; a nuclear matrix element or beta-decay rate is not computed.
mₑₑ² = a² + b² + 2ab cos χ. Changing this phase leaves the beta mass and oscillation kernel unchanged. Neither its value nor the absolute mass scale is selected by this readout.
32 paired archive streams · explicit scale choices
Bare Wilson action coordinates in GeV
These are bare Wilson parameters, not identified physical quark masses or renormalized MSbar values. The same deletion label propagates κᶜ, the ratio-tuned κ, hadron fits and the potential. Statistical error and fit sensitivity are separate; total physical uncertainty is not supplied.
| Hopping coordinate | Bare Wilson GeV | Statistical GeV | Fit sensitivity GeV |
|---|
The ratio-tuned coordinate uses the empirical pion/rho ratio; zero at κᶜ is definitional. The 0.440 GeV string assignment and 0.5 fm r₀ assignment are conventions, not exact measured physical truths.
Exact finite rank certificates
Keep the complete archive in fewer qubits
At four rounds, 48 padded archive qubits become at most 2 quantum archive qubits plus all 8 classical bits. Every admitted source vector and quantum-reference correlation can be reconstructed. This is a reversible representation, not erased history or an autonomous reset.
Every retained history and its exact quantum rank
| Original return history | Quantum rank | Original probability |
|---|
Same calibrated fermion source · supplied expansion law
Count particles through a finite expansion
The scale factor changes from 1 to 4. All twelve fermion species and antiparticles evolve in the same CAR source; the 90 complete pair factors retain cross-group correlations. The scale factor and clock are supplied. Boson production, Einstein backreaction and a physical cosmic history are not derived. Displayed bounds are rounded; the receipt retains rational enclosures.
| Conditional fermion type (both orientations) | Mean final count | Vacuum pair-creation probability |
|---|
Complete total-count law: 0 through 180
| Total count | Original probability |
|---|
Certified mixing within native bath components
For the declared reversible repair-bath extension, sufficient steps for total variation ≤ 10⁻³ are maximized across the 26 preserved components. q = exp(−2β). Component weights and the full bath history are retained.
| q | Sufficient steps |
|---|
Reference-inclusive quantum source relaxation
Sufficient collision sweeps for unhalved reduced source/reference error ≤ 10⁻⁶. This marginal bound traces the explicitly retained bath archive; the complete history does not forget the input.
| Supplied T (GeV) | Sufficient sweeps |
|---|
Ten complete finite constructions
What the executable results establish
Complete particle measurements
Identity and mass in the same readout
| Source orientation | Charge | Color C₂ | Helicity | p_z (GeV) | Measured energy (GeV) | Rest coefficient (GeV) | Unresolved rank |
|---|
Every original probe and detector outcome
| Detector group | Original probability |
|---|
Finite theorems reduce executable work
A smaller compiler with complete archives
| Original return history | Original probability |
|---|
Separate thermal constructions and their limits
Track populations across a declared thermal history
| Aggregate | Number share | Energy share |
|---|
What the native repair actually equilibrates
Particle number on the actual finite source
| Conditional type | Mean count | Share of pooled expected counts |
|---|
Couplings, flavour and composite controls
Which measurements constrain the remaining inputs?
Exact family invariants
A frequency-dependent Higgs vertex
| Source frequencies | Range of four selected normalized components |
|---|
Correlated archived hadron fit and both GeV anchors
| Observable and empirical anchor | GeV | Statistical GeV | Fit sensitivity GeV |
|---|
A constructed free-mass law
From an analyzer effect to a rest frequency
The same source and its finite precision
All 36 setting/reservoir/energy/charge records are retained, including 30 zero weights. The physical electric charge includes the reservoir and its idle compensating reference.
Inspect the complete rest-energy instrument
| Setting · reservoir output | Source electric charge | Source energy | Conditional GeV energy | Original probability |
|---|
Empirically calibrated quadratic source
Seventeen conditional mass coefficients
| Target type | Conditional coefficient (GeV) | Input convention and physical matching |
|---|
Complete particle, antiparticle and flavor readouts
| Target · orientation | Pointer / energy row | Source energy (GeV) | Reference cost (GeV) | Original probability |
|---|
Additional source candidates and gauge coordinates
Native neutral energy records
Coupled neutrino controls and a scalar-density pole
An exact neutral scalar-density response
Inspect every preparation and neutral-probe outcome
Non-ground preparation records remain terminal. The ground record is replaced by its probe children and is counted once. Failure energy is unmeasured; its probability remains in the total.
| Original record | Energy kind | Source-unit interval | Original probability interval |
|---|
All six occupation-density records
| Occupation · energy outcome | Source energy transfer | Original probability interval |
|---|
Constructed quark splitting and a scale obstruction
What separates the up and down responses?
Positive electric dressing
One common electric coefficient is 1. These source-unit shifts depend on source/reference geometry and hypercharge. They are not physical quark masses or separately fitted clocks.
Complete selected response measure, including failure
| Original record | Source / relational gap | Total gap with reference | Original probability interval |
|---|
Archived diagonal-fit composite control
Pions, nucleons and the scale choice
| Composite label | Conditional value (GeV) | Statistical (GeV) | Fit sensitivity (GeV) | Measured reference (GeV) |
|---|
One declared defect and scalar law
Which scalar response does the source select?
A selected mode and a chosen patch
The lowest free mode gives nearly equal strengths. The patch ratio near 16,385 belongs to a chosen intervention. Neither is a physical generation count or measured Yukawa hierarchy.
The filled sea responds differently
A scalar pulse reaches a fermion pair
Full native quantum contact
Propagation test: periodic defect bands
| Axis · boundary phase | Lower positive energy | Upper positive energy | Lower ΔE from Γ | Upper ΔE from Γ |
|---|
Seventeen Standard Model target types
Physical masses and calibrated action parameters
| Target label | Source physical rest mass (GeV) | Empirical action parameter (GeV) | Parameter convention and attachment |
|---|
Additional source modes and counting
Complete finite instrument
Every lepton measurement outcome
A weak round retains both cells’ return flags. Changing the number of rounds changes the finite phase and coherence; the complete outcome probabilities always sum to one.
Outcome bars use current value 1 and pair reading probability 2/9. Phase and coherence compare current values 0 and 1; the bound includes all three values. A fresh pair is supplied for each round.
One round, four outcomes
Nonreturn outcomes are part of the calculation. Their environments are retained through the reset construction.
Exact finite population law
From repair attempts to populations
Class-pair probabilities
An exact information limit
What class counts reveal
A specified thermal comparison
| Family | Number fraction | Energy fraction |
|---|
Conjugation theorem and native check
What can create an average asymmetry?
Complementing the loads and repair coins reverses every class and integer lift. Symmetric preparation with fair coins gives zero average signed class imbalance at every finite time. Individual histories can fluctuate.
Conservative bound for an observable between −1 and 1, starting from a symmetric ensemble. It is not a predicted asymmetry or a baryon-to-photon ratio.
Paired native histories
Retained lattice measurements
Shared uncertainty across masses
Masses measured on the same configurations share fluctuations. Their covariance matters when taking a difference or forming a joint comparison.
| Observable | Value | Statistical error | Fit variation |
|---|
From a mode to its measured response
Defect structure changes scalar response
Each strength occurs twice. This control contracts the complete local kernel with the selected geometric profile; it does not choose a particle generation.
Two doubled spatial strengths
Bars show log₁₀ strength from 10⁻⁶ to 1. Numerical strengths and complete complementary-mode leakage come from the frozen source calculation.
An actual charged-Higgs intervention
Scalar-cost susceptibility of the native charge sectors
| Removal channel | Complete moment M₂(1) | dM₂/dμ at μ = 1 |
|---|
Complete finite coupling records
Read a coupling from source records
Empirical calibration · comparison extension
Six quark parameters at one scale
| Calibrated family label | Running action parameter (GeV) |
|---|
Finite theorem to observer
A quotient that the observer can read
Reproduce the calculations
Each data file is copied from its owning RER receipt and bound by SHA-256. The linked proofs state the construction, its premises and the scope of each result.
Download the displayed data and source bindings ↗