Left: the repair network around one observer, from the run itself. Right: a separately prepared free Dirac packet for each selected source ID. It illustrates a proposed field readout; it is not yet the interacting field reconstructed by the load run. Follow one source ID through its wave packet and detector records below. Click a label to inspect it; drag to turn the box.
The public programs coherent-seam-repair-v1 and coherent defect wave of the theory repository, run here step by step. Twelve ports, thirty seams, twenty faces. Drag to turn the carrier.
The committed rule of the big runs stays as it is. This is the coherent version of the same seam repair: the observer keeps the removed disagreement in its own record, so nothing is erased and the quantum moves as a wave.
Two kinds of object are separated by the law itself: the vector type and the spinor type of quantum, with conserved charges −2 and +3 per level. A third kind is the flux of the link register. It is protected only relative to a boundary that is held fixed.
It is one carrier. There is no federation version of this law yet, no particle is identified and no rest mass follows. The Particles tab shows how the five levels label the known multiplets.
Carriers stand on a cubic lattice and share six seams with their neighbours. The walk carries a coherent record and a declared two-state spatial spin pointer. One tick uses three axis shifts plus the chosen rest rotation; two alternating ticks form a period. This is the candidate program CF-1 of the theory session, executed here. Drag to turn the box.
The routing step is the seam operation of the public coherent program, taken between neighbouring carriers and pointed by the spin. Along an axis a massless branch has group speed one cell per tick. For the symmetric two-tick product, the Dirac comparison has cubic error only when all momentum components and the rest angle shrink together.
Declared, not derived: the cubic arrangement, the spin as pointer, the reflection of the record, the mass step and its angle. The rest angles shown are numbers of one carrier at the scale of the lattice. They are not masses in physical units.
The mass option used here gives the two handedness partners of a particle different angles, so it cannot be the whole mass step. The other option, a toggle of the neutral spinor level, fits the particle chart and has no value yet.
The display counts individual ticks; the alternating period contains two. The rest rotation is split around the three axis shifts. On an even lattice the walk preserves four body-centred sublattices, whose probabilities are summed in the picture.
At zero rest angle the CF-1 two-tick product has 32 zero-phase nodes and 32 phase-π nodes in the full momentum zone. A low-momentum packet with uniform angle and flat links retains its momentum support. The joint scaling p = εk, θ = εm has O(ε³) one-period operator error and O(ε²) error at fixed rescaled time. Fixed θ with only p shrinking does not have that bound. Finite product proof and its domain.
Right: schematic standard thermal history with cited observations and model assumptions. Left: separate OPH proposals and executable register records. Each OPH entry says whether it is executed, stated under premises, imported or not derived. Pick an era. Below the eras: The first defects and early plasma, the executed register history beside a schematic thermal history.
The interactive panels execute three specified constructions. Step 1 applies the passive register rule on one carrier. Steps 2 and 3 use the candidate CF-1 quantum tick and its apparatus. The later cards distinguish finite amplitude identities, Hamiltonian energy lines and calibrated mass comparisons.
Twelve ports hold integer loads. Repair evens the loads across a seam; an accepted current-driven register twist changes its two adjacent face classes. Two blank faces can become a conjugate pair. Orange marks classes 1/5, amber 2/4, green 3. The quark and lepton assignments are candidate labels. Register pairs can move, annihilate, split, exchange or fuse. The register does not feed back into the load dynamics.
Two wave packets start with zero mean momentum on a one-dimensional line. Left: zero rest angle, with fronts at one cell per tick. Right: a chosen coherent rest rotation changes the phase and spreading. The internal record is not measured during this evolution. The dial reads the zero-momentum phase of that same walk; interpreting its angle as a physical particle mass requires a separate source and unit map.
A prepared quantum walk evolves on a line of 256 cells. Position records project onto disjoint groups of cells. The translation-phase detector has a complete finite-clock probability law and a declared real-amplitude state update. Each record samples an outcome and changes the state. Track mode records every detector-width ticks; coarse and fine detectors produce different disturbances. A fitted finite track slope is a detector statistic, not an undisturbed velocity or a sharp simultaneous position and momentum.
For the declared neutral background H=(0,v), the finite Yukawa benchmark gives m=|vY|, with v=v_EW/√2. A quantum scalar memory instead has its own stationary reference, two charged energy-transfer lines and complete residues. The same-H elementary/composite relation is exact in that finite memory; it does not prove a relativistic rest-mass pole or continuum FMS transfer. The masses below are comparison targets, and their physical unit is a calibration input.
Each large panel shows where one load quantum would be found, per observer cell, around the observer at the centre (white ring). The dashed circle is the supplied position detector. The grey circle is the influence front of the native repair, the farthest any record can have reached since the preparation. Each small panel is what a momentum analyser would record. All three panels start from the same preparation and share one clock, the sweep count; the observer at the centre counts about 33 own ticks per sweep.
Native record law. The current instrument of the executable-observer paper. An attempt on a seam tests one of its two ends for the quantum, the coin choosing the end. Records are diagonal in the loads, so they never measure a momentum. A superposition of positions turns into entanglement with the tapes at 5 to 6 per sweep, and the position law diffuses.
Transfer continuation. Declared. The unitary group whose generator is the generator of the native transfer. The quantum moves like a particle of fixed inertial mass and its packet spreads.
Admitted wave. Declared. The positive-frequency part of the coherent wave of the paper, driven seam by seam: one event turns the seam variable and the difference of its two ports by the pulse angle. All wave numbers move at one speed, proportional to the pulse angle and below the influence front. On a regular clock the wave keeps going. Under the declared schedule of independent random draws the count noise of the schedule scatters it within about one over the pulse angle in mesh edges. On the paper clock the speed halves with every refinement level.