Relational Field Theory

The Relational Punnett Square: Mapping the Four States of the Field

Once you realize that Parallility (internal multi‑threading) and Plurallility (relational multi‑relating) are orthogonal dimensions, something remarkable happens:

You can map them.

Not metaphorically.
Not poetically.
Literally.

Two independent axes create a matrix — a relational Punnett square that reveals the four fundamental states a person or system can occupy in the field.

This is the moment where Relational Field Theory becomes a coordinate system.

The Two Axes

Axis 1 — Internal Architecture

Parallile (multi‑threaded internal self)
Singular (single‑threaded internal self)

Axis 2 — Relational Field State

Relate (coherent, attuned, mutually shaping)
Disrelate (incoherent, misaligned, low‑bandwidth)

These axes are independent.
They do not cause each other.
They can amplify each other, contradict each other, or exist in any combination.

And when you cross them, you get the four basic relational states.

The Relational Punnett Square

This matrix is deceptively simple.
It explains:

why some parallile people struggle relationally
why some singular people are extraordinary connectors
why internal multiplicity doesn’t guarantee relational multiplicity
why relational multiplicity doesn’t require internal multiplicity
why two people can look “the same” from the outside but be operating from completely different architectures

This is the first time the theory becomes visible.

Why This Matters

Once you have the matrix, you can:

locate yourself
locate others
locate systems
diagnose relational states
predict field behavior
understand misattunement without moralizing it

This is the foundation for the next layer — the realization that there are more orthogonal axes shaping the field, including anchoring and power source.

Those axes expand the matrix into a multidimensional relational space — the beginnings of a full relational physics.

Next up:
Two More Axes — Anchoring and Power Source.