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Locality, Probability and the Relevance of History

This paper proposes a generalized locality constraint for probabilistic theories where event probabilities are determined by past probabilities, arguing that Bell-inequality-violating quantum phenomena are compatible with relativity and realism because they demonstrate the relevance, rather than the irrelevance, of history.

Original authors: Sebastian Horvat

Published 2026-11-02
📖 7 min read🧠 Deep dive

Original authors: Sebastian Horvat

Original paper licensed under CC BY 4.0 (http://creativecommons.org/licenses/by/4.0/). ✨ This is an AI-generated explanation of the paper below. It is not written or endorsed by the authors. For technical accuracy, refer to the original paper. Read full disclaimer

In the vast landscape of modern physics, two towering pillars stand side by side, yet they often seem to speak different languages. One is the theory of relativity, which teaches us that nothing can travel faster than light and that causes must precede their effects in a strict, local order. The other is quantum mechanics, the rulebook for the subatomic world, which describes a reality where particles can be linked across vast distances in ways that seem to defy that same local order. For decades, this tension has been sharpened by a famous puzzle known as Bell's theorem. This theorem suggests that if the universe follows the rules of relativity and if particles have definite properties before we measure them, then certain statistical patterns in experiments should never occur. Yet, in laboratories around the world, those patterns do occur. The universe appears to be breaking the rules of local cause and effect, forcing physicists to choose between abandoning the idea that causes are local or accepting that the universe is stranger than we thought.

A new paper by philosopher Sebastian Horvat offers a different way to look at this puzzle. Instead of choosing between locality and the strange behavior of quantum particles, Horvat suggests that our understanding of how history influences the future might be the part that needs adjusting. He proposes that the conflict arises not because nature is non-local, but because we have been assuming that the past is irrelevant to the present in a specific, technical sense. By redefining what it means for a theory to be "local" in a probabilistic world, Horvat argues that quantum phenomena can remain perfectly local without violating the speed of light, provided we accept that the full story of how a situation came to be matters more than we previously believed.

To understand the shift, one must first see how the old rules were written. For a long time, physicists believed that if you knew everything happening in the immediate past of an event, you could determine exactly what would happen next. This is the idea of functional determination: the present is a direct result of the immediate past. However, quantum mechanics is not deterministic; it deals in probabilities. You cannot say with certainty where an electron will land, only how likely it is to land in various spots. To accommodate this, the famous physicist John Bell proposed a modified rule. He suggested that while the past might not determine the exact outcome, it should determine the probability of that outcome. In Bell's view, if you know the state of the immediate past, the probability of an event happening here should not change, no matter what is happening far away in a place that light cannot reach. This became the standard test for "local causality."

Horvat argues that Bell's test, while logical, misses a crucial nuance when applied to a world of probabilities. He points out that Bell's rule treats each possible scenario in isolation. It asks: "Given this specific past, what is the probability of this future?" But Horvat suggests that a more natural way to generalize the idea of local determination is to look at how probabilities themselves relate to one another across different possible histories. In his view, a truly local theory should ensure that the probability distribution of an event is determined by the probability distribution of events in its immediate past. It is a subtle but profound shift: instead of events determining other events, or events determining probabilities, the distributions of possibilities determine the distributions of future possibilities.

When Horvat applies this new, more flexible definition of locality to the data, a surprising result emerges. The strange correlations seen in quantum experiments, which violate Bell's inequalities, do not necessarily break this new rule. The violation only happens if we hold onto an extra, hidden assumption: the idea that history is irrelevant. This assumption, which physicists often take for granted, is the belief that once you know the current state of a system, the specific path it took to get there does not matter for predicting its future. It is the belief that the present moment contains all the necessary information, and the past is just a forgotten story.

Horvat demonstrates that if you drop this assumption, the conflict disappears. He proposes that the future probability of an event can depend on the history of how the current state was reached. To visualize this, imagine a red cube appearing in a room. If you assume history is irrelevant, you would predict its future behavior based solely on the fact that it is a red cube right now, regardless of how it got there. But if history is relevant, the cube's future might depend on whether it arrived from a red pyramid or a red sphere. In the quantum world, the "red cube" is a measurement outcome, and its "history" includes the specific chain of events that led to the entangled particles being in the state they are in. The paper suggests that the correlations we see are not magic connections across space, but the result of the fact that the current state carries a memory of its specific origin.

This does not mean that causes travel backward in time or that the future changes the past. Rather, it means that the probability of what happens next is not fixed solely by the snapshot of the present, but is refined by the full context of how that snapshot was formed. The paper argues that the universe is not "Markovian," a technical term for systems where the future depends only on the present. Instead, the universe is sensitive to its own history. The probability of an event is determined by the probability of the events in its immediate past, but that past probability distribution itself is shaped by the deeper history. This allows the theory to respect the speed of light and the local nature of cause and effect, while still accounting for the spooky connections that quantum mechanics reveals.

The implications of this view are significant for how we understand reality. It suggests that the "spooky action at a distance" that Einstein famously disliked might be an illusion created by ignoring the relevance of history. If we accept that the past matters, we can keep the comforting idea that causes are local and that nothing travels faster than light. The paper does not claim to have solved every mystery of quantum mechanics, nor does it provide a complete new theory of the universe. Instead, it offers a new logical framework that removes the contradiction between relativity and quantum mechanics. It suggests that the path forward lies not in abandoning locality, but in recognizing that the story of how we got here is essential to understanding where we are going.

In the end, this work invites us to rethink the nature of time and causality. It proposes that the universe is a tapestry where the threads of the past are woven into the probabilities of the future. By acknowledging that history is relevant, we can reconcile the two great pillars of physics without sacrificing the fundamental principle that causes are local. The paper leaves us with the possibility that a local, realistic theory of the quantum world is still within reach, provided we are willing to listen to the full story of the past, not just the present moment.

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