Relying on some auxiliary assumptions, usually considered mild, Bell's theorem proves that no local theory can reproduce all the predictions of quantum mechanics. In this work, we introduce a fully local, superdeterministic model that, by explicitly violating settings independence-one of these auxiliary assumptions, requiring statistical independence between measurement settings and systems to be measured-is able to reproduce all the predictions of quantum mechanics. Moreover, we show that, contrary to widespread expectations, our model can break settings independence without an initial state that is too complex to handle, without visibly losing all explanatory power and without outright nullifying all of experimental science. Still, we argue that our model is unnecessarily complicated and does not offer true advantages over its nonlocal competitors. We conclude that, while our model does not appear to be a viable contender to their non-local counterparts, it provides the ideal framework to advance the debate over violations of statistical independence via the superdeterministic route.Aclaró que un Aleph es uno de los puntos del espacio que contienen todos los puntos.-Jorge Luis Borges ...il s'ensuit, que cette communication va à quelque distance que ce soit. Et par conséquent tout corps se ressent de tout ce qui se fait dans l'univers; tellement que celui qui voit tout, pourrait lire dans chacun ce qui se fait partout...-Gottfried Wilhelm Leibniz
Bell's theoremWe start this section with an overview of Bell's theorem (see Myrvold et al. (2019); Goldstein et al. (2011) for thorough discussions). Then we make a few comments regarding the relation between locality and factorizability that will be relevant for the settings independence discussion later on.
The inequalityConsider an ensemble of pairs of particles, all created in the state that quantum mechanics describes as a singlet. Particles of each pair are sent to two spatially separated locations, 1 and 2, where spin measurements are to be performed. Let a, b denote the spin directions measured in 1 and 2, respectively, and let A, B stand for the corresponding results (with spin-up corresponding to +1 and spin-down to −1). Denote by λ the complete, fundamental, state of each pair; that is, λ contains complete information