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This study calculates the maximum quantum violation of locality in Hardy's test, finding it achievable with two-qubit systems. Higher-dimensional systems offer no advantage for this quantum nonlocality test.

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Area of Science:

  • Quantum Information Theory
  • Foundations of Quantum Mechanics

Background:

  • Hardy's test is a key protocol for demonstrating quantum nonlocality.
  • Tsirelson's bound quantifies the maximum violation of Bell inequalities achievable in quantum mechanics.
  • Understanding the limits of nonlocality is crucial for quantum information processing.

Purpose of the Study:

  • To compute an analogue of Tsirelson's bound for Hardy's test, applicable across all system dimensions.
  • To identify the quantum states capable of achieving this maximal violation.
  • To investigate the role of system dimension in experimental implementations of Hardy's test.

Main Methods:

  • Analytical computation of a nonlocality bound analogous to Tsirelson's bound for Hardy's test.
  • Characterization of quantum states that saturate the derived bound.
  • Analysis of device-independent upper bounds under realistic constraints.

Main Results:

  • The maximum violation of locality in Hardy's test is dimension-independent and matches the value for two-qubit systems.
  • Only a specific class of quantum states achieves this maximal violation, enabling device-independent self-testing.
  • Realistic constraints do not alter the advantage of two-qubit systems; higher dimensions offer no benefit.

Conclusions:

  • Hardy's test, even with realistic constraints, is optimally implemented using two-qubit systems.
  • The findings highlight the efficiency of two-qubit systems for device-independent self-testing of specific quantum states.
  • This research provides fundamental insights into the limits of quantum nonlocality and its experimental realization.