When searching for additional insights I found in: Laidlaw A. “An Unspeakable Mechanism”. Intl. J. Adv. Res. Phys. Sci. (2018), 5, 6, 10-28: “local realist field model,” “distributed action” and “Fields at different points in space do not interact with each other. Alternatively, at any given space point, the interaction between two fields depends only on the values of the fields that are present at that point.”

I also found in A. Laidlaw and L.G. van Willigenburg “On the Appearance of Action at a Distance” https://www.researchgate.net/publication/372841182: “If we are to think of the interaction quanta as distributed fields then we must also think of the source and the target quanta as distributed fields. Each of them permeates the entire space, which is also the modern view from Quantum Field Theories. The source and the target are thus always touching, everywhere.”

And “Therefore, what the QED interaction mechanism is describing is a distributed transfer of energy-momentum from one distributed field to another. In other words, it is describing local field-field interactions that are spatially distributed, not atomist particle-particle interactions. It is describing distributed action.”

Proposal

Distributed fields are formed from the primal state of the universe in an epoch. Whether one considers details of the universe as having expanded from some compact primal energy state, or considers that the details have condensed from a universe-scale primal energy state (my favorite), each “distributed field” is of universe scale. On the occasion of two distributed fields interacting, their interaction occurs in their full extent. An observable is a sample of the interacting distributed fields at any space point of that interaction. The location of the space point of an observation is determined by an observer sampling the interacting fields from one of them.

Were we to accept neutrality of the universe, we would find that for each distributed field a complementary distributed field exists. Further, we would require that interacting fields be complementary, like a key and a lock. Then, in the EPR Alice and Bob event, the two interacting distributed fields that individually include Alice’s and Bob's local states would be complementary fields. Observables of the state of Alice's and Bob's complementary distributed fields would occur under the influence of the values of the fields at each observation point, including from which distributed field the observation is made. The observation determines the state of Alice's distributed field, and of necessity, it also determines the state of Bob's complementary distributed field.

Now, it is specifically proposed that Alice's distributed fields are selected from a myriad of distributed fields by the location of Alice's observation. Bob's complementary distributed fields are also selected from a myriad of distributed fields by the location of Bob's observation apparatus. Setting the states of a pair of these fields that include both locations awaits setting of one field state by an observation. At the observation by Alice her distributed field is set and distributed field interaction sets Bob's distributed field to the complement of Alice’s distributed field. How? At the observation by Bob the complementary distributed field is observed, producing for instance, spin opposite.

Replies

Please inform me whether this view is on track for “distributed action.” I have been interested in non-locality for decades with a past bias toward “backward in time” anti-particle communication. I would like to understand the distributed action view also, since it seems more in line with modern treatments of non-locality.

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