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The quantum supremum of the I3322I_{3322} Bell inequality is not attained in finite dimension

This paper proves that the quantum supremum of the I3322I_{3322} Bell inequality is not attainable by any finite-dimensional strategy, demonstrating that the set of finite-dimensional quantum correlations is not closed in the (3,3,2,2)(3,3,2,2) scenario and requires unbounded local dimensions to approach the maximum value.

Original authors: Jef Pauwels

Published 2026-09-01
📖 5 min read🧠 Deep dive

Original authors: Jef Pauwels

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 strange and counterintuitive world of quantum physics, particles can become linked in ways that seem to defy the rules of everyday experience. This phenomenon, known as entanglement, allows two separated objects to share a single existence, where measuring one instantly reveals information about the other, no matter how far apart they are. Scientists have long used mathematical tests, called Bell inequalities, to check if these connections are truly quantum or if they could be explained by hidden, classical rules. These tests act like a boundary line: if the results stay on one side, the world behaves classically; if they cross over, the universe is behaving in a genuinely quantum way. For decades, physicists have wondered if there is a limit to how strongly these quantum connections can be tested. Specifically, they asked whether there is a maximum possible score for these tests that can be reached with a finite amount of quantum resources, or if the best possible score is a theoretical ceiling that can only be approached by using an infinite amount of resources.

A recent study by Jef Pauwels, a physicist at the University of Geneva and Constructor University, settles a long-standing debate about one of these specific tests, known as the I3322 inequality. This test involves two people, traditionally called Alice and Bob, who each have three different choices of measurements to make, with each choice yielding one of two possible outcomes. In 2010, researchers Pál and Vértesi discovered a clever way to construct quantum strategies for this test using states of increasing size. They found that as they made the quantum systems larger and more complex, the test scores kept getting higher, inching closer to a specific number roughly equal to 0.25087538. They suspected that this number was the absolute limit, but they also guessed that no matter how large they made their quantum system, they could never actually reach that exact number. They believed the limit existed, but it was forever out of reach for any finite machine.

Pauwels has now proven that Pál and Vértesi were correct on both counts. The study demonstrates that the highest possible score for this test is indeed that specific number, but it also proves that no quantum strategy built from a finite number of dimensions can ever achieve it. To reach the limit, one would need a system with an unbounded, or infinite, local dimension. This finding is significant because it reveals a fundamental gap in our understanding of quantum correlations. It shows that the set of all possible outcomes from finite quantum systems is not "closed," meaning there are limit points that the systems can get arbitrarily close to but never actually touch. In the specific scenario of three settings and two outcomes for each person, this is the smallest possible setup where this strange behavior occurs.

The proof relies on a method of translating the complex quantum problem into a simpler, more manageable form. The researcher took any possible strategy Alice and Bob could use and mapped it onto a grid of probabilities that describes how their measurement settings relate to each other. This grid acts as a ceiling, providing an upper bound on the score they can achieve. The study then showed that the strategies found by Pál and Vértesi, which use a repeating pattern of connections, are the most efficient way to climb toward this ceiling. As the size of the quantum system grows, these strategies get closer and closer to the limit. However, the mathematical conditions required to hit the limit exactly would force the quantum state to become impossible to normalize, essentially meaning the state would require infinite energy or probability to exist. Therefore, the perfect score remains a horizon that finite systems can chase but never catch.

This result has immediate consequences for how we understand the limits of quantum mechanics. It confirms that to get arbitrarily close to the maximum violation of this inequality, one must be willing to use quantum systems of ever-increasing size. There is no fixed size of quantum computer or particle system that can produce the maximum possible correlation for this test. The study also clarifies the landscape of quantum correlations, showing that the collection of all finite-dimensional quantum behaviors is distinct from the collection of all possible quantum behaviors, including those that might require infinite dimensions. While the paper leaves open the question of whether an infinite-dimensional system could actually reach the limit, it firmly establishes that finite systems cannot.

The work was formalized using a computer proof assistant, a tool that checks mathematical arguments with absolute precision to ensure no logical errors exist. This rigorous approach confirms that the result is not just a numerical observation or a simulation, but a mathematical certainty. The findings suggest that the boundary between what is possible with finite resources and what is possible in the broader quantum world is sharper and more complex than previously thought. For experimentalists, this means that any attempt to reach the theoretical maximum of this test will always fall slightly short, no matter how sophisticated their equipment becomes. The limit is real, but it is a destination that finite quantum systems are fundamentally unable to reach.

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