Peter,
Looked again a couple times at Traill's essay. Perhaps starting to get the connection Terry Bollinger was trying to point out.
From perspective of the geometric wavefunction interaction (GWI) model Michaele and I are working with two essential points relevant to Declan's essay seem to stand out.
1. There exist two different varieties of quantized impedances - scale invariant and scale dependent. Forces associated with invariant impedances can do no work, cannot share energy/information. Resulting motion is perpendicular to direction of applied force. These are the conduits of non-locality. They communicate only the quantum phase of entanglement, not a single measurement observable. Here the GWI approach appears to be in harmony with what Declan shows.
2. What distinguishes quantum from classical is quantum phase. Once one accounts for the fact that phase is not a single measurement observable, from the perspective of our synthesis of geometric wavefunction interactions with quantized impedance networks QM appears 'classical', again in agreement with Declan's conclusion.
Having arrived at this, now feel ready to take a look at Watson, and then yours again. Tho we're not math folks here, Poincare sphere is only slightly familiar to me from Penrose's road to reality.