Graduate The wave-function as a true ensemble

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The discussion critiques the ψ-ontic/epistemic distinction, arguing it inadequately identifies ensemble interpretations of quantum mechanics. A new definition is proposed, highlighting that all ψ-ensemble interpretations that align with quantum mechanics violate Statistical Independence. The conversation also addresses the flexibility of defining 'ontic' variables, suggesting that such malleability undermines the robustness of theoretical foundations. Additionally, a misinterpretation regarding observables related to quantum states is corrected, clarifying that only pure states orthogonal to a given state will yield certain predictions. The insights emphasize the complexities in defining wave-functions and their implications for quantum theory.
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"We argue that the ψ-ontic/epistemic distinction fails to properly identify ensemble interpretations and propose a more useful definition. We then show that all ψ-ensemble interpretations which reproduce quantum mechanics violate Statistical Independence."

https://arxiv.org/abs/2109.02676
 
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"Suppose you have a theory that isn’t ontic because two of the hidden variables map to the same wave-function. Well, then you can just declare the wave-function to be part of the hidden variables, so that the new hidden variables – now including the wave-function – will always map to only one wave-function. Such an easily malleable definition of ‘ontic’ is not what one wants to base theorems on."

This is an interesting point. If I have a quantum state ##\psi##, I can always define an observable $$\hat{O} = \lambda_\psi|\psi\rangle\langle\psi| + \lambda_{\not\psi}(\hat{I} - |\psi\rangle\langle\psi|)$$ We have a property ##\lambda_\psi## resolvable (in principle) by experiment, that ##\psi## predicts with certainty. All other pure states will predict ##\lambda_{\not\psi}## with certainty. Make this variable a real hidden variable and voila, your wavefunction uniquely characterises the physical state of the system.
 
Morbert said:
"All other pure states will predict ##\lambda_{\not\psi}## with certainty.
No, they won't. Only pure states orthogonal to ##\psi## will.
 
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Oops stupid mistake
 
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I am slowly going through the book 'What Is a Quantum Field Theory?' by Michel Talagrand. I came across the following quote: One does not" prove” the basic principles of Quantum Mechanics. The ultimate test for a model is the agreement of its predictions with experiments. Although it may seem trite, it does fit in with my modelling view of QM. The more I think about it, the more I believe it could be saying something quite profound. For example, precisely what is the justification of...

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