in the thread https://groups.google.com/g/Bell_quantum_foundations/c/pt04xzq9W28 Richard introduced the co-authored paper (https://arxiv.org/abs/2605.13154 )Three ways to find comfort with the Bell proof and the results of the Bell experiments.
Attached is my reply, Reply-to_Gill_Helland_Jongejan.pdf, proposing a fourth way.
The starting point is an ontological one: a nilpotent universe that preserves the whole, which cannot change by local interactions. The role of the optical apparatus in Freedman–Clauser, Ou–Mandel and Kwiat et al. is not to create entanglement but to establish the conditions under which it becomes expressible in polarisation correlations. What Hilbert space represents as wave-function collapse is proposed to be the local expression of a globally constrained physical event.
The proposal comes with a go/no-go experiment. Unlike the three positions surveyed, which are empirically equivalent to standard quantum mechanics and to one another by construction, this one predicts a CHSH violation where standard quantum mechanics predicts none. A null result, that is S<2, rejects my proposal.
The discussion I am after is whether a nilpotent constraint is viable against Hilbert-space constructions, and whether it is a fourth way in the sense of Richard, Inge and Bart. Pushback on the argument is welcome — the paper states in §4.8 exactly what would refute it. Constructive additions to harden the argument are welcome too.
PS — please do not hijack the thread with pet theories.
Regards
Anton
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On 17 Jul 2026, at 20:26, anton vrba <anto...@gmail.com> wrote:
<Reply-to_Gill_Helland_Jongejan.pdf>


Dear Richard,
You are right — inaccessibility doesn't distinguish the cases, and the sentence claims too much. Rather than defend it, let me propose the replacement and ask whether you'd accept it.
I would cut the "third case" sentence and put in its place:
This randomness is reducible to initial conditions in Gill's sense, and I do not dispute that. But the underlying variable is not local: the steering makes the second outcome depend on the first analyser's setting, so there is no λ with X = f(a,λ) and Y = g(b,λ) separately — the factorisation Bell's derivation requires. The framework is therefore a nonlocal, deterministic, no-signalling pilot-wave theory. That is a known category, not a new one; what is new, if anything, is the specific guidance law and the experiment that would test it, not the metaphysical slot it occupies.
This concedes your point, drops the overreach, and rests the distinction on local versus nonlocal reducibility rather than on accessibility. I recognise you may still say a nonlocal deterministic HV is just the action-at-a-distance route you've already declined — in which case the honest position is that the novelty is the guidance law and the test, nothing more.
Does that edit satisfy the objection on your side of it?
Anton
On 18 Jul 2026, at 10:47, Inge Svein Helland <in...@math.uio.no> wrote:

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