
constraint — and it is not an invention of this paper: the published crystallization simulation
takes exactly a triangle as its initial condition (Ref. [26],
§
2.3). This paper supplies the seed’s
standing: why a triangle, and why it persists. [conjectured]
4. The first clock. Regularity is an output, not an input: before the triangle there are no in-
tervals to be regular in. The surviving rulebook must be rule-invariant: the same law at every
application, since a drifting rule cannot accumulate. Given invariance, the triangle’s verifica-
tion cycle defines the first interval. The uniformity of physical law is a survival requirement,
not a happy fact. [conjectured]
5. Sheet growth and the periodic lift. Growth is clocked: attachment attempts are ran-
dom, and commits happen at verification ticks. Randomness proposes; order disposes. One
dimensionless parameter enters here, the first the genesis regime admits: the attempt rate µ,
attachments presenting per verification cycle, denominated in the structure’s own clock since
no other exists. It has a published cousin: the simulation already runs with a stochastic lift
probability (P
lift
, Ref. [26],
§
2.3), so growth-parameter dependence is not foreign to the proto-
col. A frequency of the pre-triangle fluctuations themselves would be ill-posed — no clock, no
volume — but once the first cycle ticks, µ is legal, and it governs two things: the front speed,
which saturates at the one-layer-per-cycle ceiling when attempts are abundant, and plausibly
the trapping rate, since a crowded boundary means competing attachments and more rem-
nant nodes caught as each layer closes. The front advances at most one layer per cycle, a
maximum propagation speed built into construction. In-plane extension continues the trian-
gle into the triangular sheet, precisely the close-packed (111) plane of the eventual crystal.
The projection that fixes S = A/4ℓ
2
P
in Ref. [28] is therefore taken along the oldest structure
in existence. The periodic lift adds nodes in the hollows above or below the sheet: not matter,
just the forming material of the adjacent layer, each new node completing a tetrahedron with
the three beneath it and opening the third dimension. This growth sequence (seed, sheet,
lift) is the published simulation’s own protocol (Ref. [26],
§
2.3), feeding its K = 4 → K = 12
transition; matter arises exactly where that paper puts it, in remnant nodes trapped during
the transition, and nowhere in the lift. What this paper adds is the clocked reading: the
tick-gated commits, the parameter µ, and the speed ceiling. Why the sheet is triangular is,
in fact, already answered in print: the published simulation derives in-plane coordination
six as “the maximum coordination consistent with strict planarity” (Ref. [26],
§
2.3). The
residual open question is smaller: why growth is planarity-first, sheet before lift, rather than
three-dimensional from the start. Also open is the dependence of defect density on µ: if
simulation shows the trapping rate to be monotone in attempts per cycle, the abundance of
matter becomes a fossil record of how busy the pre-geometric substrate was, an inheritance
of exactly the kind the screening argument of
§
11 permits. [the seed, growth, lift, transition,
and trapping are published; the clocked reading and µ are this paper’s]
6. The published middle. The transition, the defects, the vacancy sector, the survival cut-
off [26, 27, 28]. [published]
7. The ends (
§
8). [conjectured reading]
7 The emergence schedule
The other laws of physics do not switch on together; they switch on as the structures that define
them come into existence, and for three rungs of the ladder the mechanism is an established theorem
6