Abstract

We propose a scheme for the detection of qubit–environment entanglement which requires only operations and measurements on the qubit, all within reach of current experimental state-of-the-art. The scheme works for any type of interaction which leads to pure dephasing of the qubit as long as the initial qubit state is pure. The scheme is direct in the sense that it allows the detection of entanglement present in the system at time tau after the initialization of the qubit in a superposition state. It requires a measurement on the qubit at time tau and a comparison of the post-measurement evolution to the evolution obtained by a modified scheme. It becomes particularly simple when one of the qubit states is neutral with respect to the environment, such as in case of the most common choice of the NV center spin qubit or for excitonic charge qubits, when the environment is initially at thermal equilibrium. In this case, the post-measurement evolution needs to be compared only to the standard decoherence which is obtained without any qubit manipulation after the preparation of the initial state.

Highlights

  • The accessibility of entanglement in larger bipartite systems is very limited up to date, because contrarily to entanglement between two qubits [1,2,3], the theoretical means for the study of such entanglement are very limited unless the joint system state is pure

  • We have proposed a scheme for the detection of qubit–environment entanglement (QEE) at a certain time τ which requires the comparison of qubit evolution after a measurement performed at said time τ with

  • The procedure is qualitatively different from the one proposed before [41] in the fact that it detects entanglement present in the system during its operation, when the results are compared to the ones obtained during another measurement

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Summary

Introduction

The accessibility of entanglement in larger bipartite systems is very limited up to date, because contrarily to entanglement between two qubits [1,2,3], the theoretical means for the study of such entanglement are very limited unless the joint system state is pure.

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The interaction
Criterion of qubit–environment entanglement
The scheme
Evolution of the system with intermediate measurement at time
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Evolution of the comparative system
The quantity of interest
Asymmetric interaction
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Example: charge qubit and phonons
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Conclusion
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