CHSH inequality

Introduction

The CHSH inequality, named after physicists John Clauser, Michael Horne, Abner Shimony, and Richard Holt, is a cornerstone of quantum mechanics and quantum information theory. It is a specific form of Bell's inequality, which is used to test the predictions of quantum mechanics against those of classical physics, particularly local realism. The CHSH inequality provides a quantitative measure to distinguish between quantum entanglement and classical correlations.

Historical Context

The CHSH inequality was formulated in 1969 as an extension of John Bell's original inequality, which was introduced in 1964. Bell's theorem demonstrated that no local hidden variable theories could reproduce all the predictions of quantum mechanics. The CHSH inequality was designed to be experimentally testable and has been a critical tool in numerous experiments that have confirmed the non-local nature of quantum mechanics.

Mathematical Formulation

The CHSH inequality involves four measurements on a pair of entangled particles. Let \( A \) and \( A' \) be two possible measurements on the first particle, and \( B \) and \( B' \) be two possible measurements on the second particle. Each measurement can yield outcomes of either +1 or -1. The CHSH inequality is expressed as:

\[ | \langle AB \rangle + \langle AB' \rangle + \langle A'B \rangle - \langle A'B' \rangle | \leq 2 \]

Here, \( \langle AB \rangle \) denotes the expectation value of the product of the outcomes of measurements \( A \) and \( B \). According to quantum mechanics, the maximum value of the left-hand side can reach \( 2\sqrt{2} \), a violation of the classical bound of 2, indicating the presence of quantum entanglement.

Experimental Verification

The CHSH inequality has been tested in numerous experiments involving entangled photons, electrons, and other particles. One of the most famous experiments was conducted by Alain Aspect in 1982, which provided strong evidence against local hidden variable theories. Modern experiments continue to close loopholes and refine the precision of these tests.

Two entangled particles emitting light in opposite directions.

Implications for Quantum Mechanics

The violation of the CHSH inequality has profound implications for our understanding of reality. It implies that quantum mechanics cannot be explained by any local hidden variable theory, supporting the idea that entangled particles exhibit non-local correlations. This non-locality is a fundamental feature of quantum mechanics and has led to the development of quantum technologies such as quantum cryptography and quantum computing.

Quantum Information Theory

In quantum information theory, the CHSH inequality is used to quantify the strength of entanglement between particles. It serves as a benchmark for the performance of quantum communication protocols and quantum algorithms. The degree to which the CHSH inequality is violated can be used to certify the security of quantum key distribution schemes.

Theoretical Extensions

Several extensions of the CHSH inequality have been proposed to accommodate different scenarios and more complex systems. These include the chained Bell inequalities, which involve more measurement settings, and the multi-partite Bell inequalities, which extend the concept to systems with more than two particles. These extensions provide a richer framework for exploring the boundaries of quantum mechanics and its applications.

See Also

• Bell's Theorem
• Quantum Entanglement
• Quantum Nonlocality
• Quantum Cryptography
• Quantum Computing