Abstract

In quantum information, lifting is a systematic procedure that can be used to derive---when provided with a seed Bell inequality---other Bell inequalities applicable in more complicated Bell scenarios. It is known that the procedure of lifting introduced by Pironio [J. Math. Phys. A 46, 062112 (2005)] preserves the facet-defining property of a Bell inequality. Lifted Bell inequalities therefore represent a broad class of Bell inequalities that can be found in {\em all} Bell scenarios. Here, we show that the maximal value of {\em any} lifted Bell inequality is preserved for both the set of nonsignaling correlations and quantum correlations. Despite the degeneracy in the maximizers of such inequalities, we show that the ability to self-test a quantum state is preserved under these lifting operations. In addition, except for outcome-lifting, local measurements that are self-testable using the original Bell inequality---despite the degeneracy---can also be self-tested using {\em any} lifted Bell inequality derived therefrom. While it is not possible to self-test {\em all} the positive-operator-valued measure elements using an outcome-lifted Bell inequality, we show that partial, but robust self-testing statements on the underlying measurements can nonetheless be made from the quantum violation of these lifted inequalities. We also highlight the implication of our observations on the usefulness of using lifted Bell-like inequalities as a device-independent witnesses for entanglement depth. The impact of the aforementioned degeneracy on the geometry of the quantum set of correlations is briefly discussed.

Highlights

  • Inspired by the thought-provoking paper of Einstein, Podolsky, and Rosen [1], Bell derived [2]—based on wellaccepted classical intuitions—an inequality constraining the correlations between local measurement outcomes on two distant systems

  • While it is not possible to self-test all the positive-operator-valued measure elements using an outcome-lifted Bell inequality, we show that partial, but robust self-testing statements on the underlying measurements can be made from the quantum violation of these lifted inequalities

  • As introduced by Pironio [41], is a procedure that allows one to systematically construct Bell inequalities for all Bell scenarios starting from a Bell inequality applicable to a simpler scenario

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Summary

INTRODUCTION

Inspired by the thought-provoking paper of Einstein, Podolsky, and Rosen [1], Bell derived [2]—based on wellaccepted classical intuitions—an inequality constraining the correlations between local measurement outcomes on two distant systems. He further showed that the so-called Bell inequality can be violated by quantum theory using local but incompatible measurements on entangled states. Mayers and Yao [6,7] showed that certain extremal quantum correlation enables the possibility to self-test quantum devices. Examples illustrating the nonuniqueness of the maximizers of lifted Bell inequalities, as well as their implications on the geometry of the quantum set of correlations are provided in the Appendixes

Bell scenario
Self-testing
MAXIMAL VIOLATION OF LIFTED BELL INEQUALITIES AND ITS IMPLICATIONS
More inputs
More outcomes
Preservation of quantum and nonsignaling violation
Implications on self-testing
More parties
Implications on device-independent certification of entanglement depth
CONCLUDING REMARKS
Lifting of inputs
Lifting of outcomes
Lifting of party
Grouping of outcomes
Splitting of outcomes
Robust self-testing of the reference state
Robust self-testing of Alice’s POVM
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