Named factors and the three maps

For each model $i=1,2,3$, retain the separate matter space ${\mathcal{H}}_i$. Add three finite named carrier factors $L_1,L_2,L_3$. They are not a spatial tensor factorization of the continuum field. Their fixed locations mark the three developing rods.

Use one total consumed context

Here $C_T$ is finite time-code memory and $C_B$ is the Ramsey probe. Taking $d_T$ a power of two gives a finite qubit encoding. The retained context is

Both clock/probe components are consumed by the complete readout.

The dictionaries are:

1. Time map. A fixed injective calibration

   $${\gamma }_T:k⟼T_k.$$

   The binary outcome $s$ is not another value of the event time. A separate history map $\kappa$ may assign $k$ to a labelled history event.

2. Location map. A map $\ell$ sends each admitted finite carrier name and tick to a point of the regular spatial slice. Its three numerical rod coordinates are $y\circ \ell$, using (eq:dev). The field module ${\mathcal{H}}_i$ remains a global represented module; this map does not localize every one of its modes at the probe.

3. Causal-wire map. For every certified scheduled dependency $a\to b$,

   $${\ell }_{\mathrm{event}}(b)\in J_g^{+}\left({\ell }_{\mathrm{event}}(a)\right).$$

   Equivalently, an ancestor of an output belongs to the metric past of that output.

These are written maps in one declared model. They are not inferred from similarity of terminology between manuscripts.