Abstract

We consider the characterization of quantum superposition states beyond the pattern ‘dead and alive’. We propose a measure that is applicable to superpositions of multiple macroscopically distinct states, superpositions with different weights as well as mixed states. The measure is based on the mutual information to characterize the distinguishability between the multiple branches of the superposition. This allows us to overcome limitations of previous proposals, and to bridge the gap between general measures for macroscopic quantumness and measures for Schrödinger-cat type superpositions. We discuss a number of relevant examples, provide an alternative definition using basis-dependent quantum discord and reveal connections to other proposals in the literature. Finally, we also show the connection between the size of quantum states as quantified by our measure and their vulnerability to noise.

Highlights

  • When going from single microscopic particles to composite systems with many degrees of freedom, quantum mechanics shows enormous complexity

  • We propose a measure that is applicable to superpositions of multiple states with unequal weights and is readily extendable to mixed states, thereby overcoming the shortcomings of previous proposals

  • We formalize this idea into a general measure that is useful for mixed states

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Summary

22 January 2018

Pavel Sekatski1,4, Benjamin Yadin2, Marc-Olivier Renou3, Wolfgang Dür1, Nicolas Gisin3 and Florian Fröwis3 Original content from this Keywords: macrospic quantum effects and states, quantum to classical transition, Schrödinger-cat work may be used under the terms of the Creative Commons Attribution 3.0 licence.

Introduction
Macroscopically extractable information
Model of a coarse-grained measurement
Role of b and calibration of the measure
Mixed states and convex roof
Alternatives and comparison
Direct convex-roof extension of the MI
Example: superpositions of coherent states Given a real α consider the state
Implications on fragility
D X acting on the macroscopic part of the state
Conclusion and discussion
Full Text
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