Abstract

We present a framework that formulates the quest for the most efficient quantum state tomography (QST) measurement set as an optimization problem which can be solved numerically, where the optimization goal is the maximization of the information gain. This approach can be applied to a broad spectrum of relevant setups including measurements restricted to a subsystem. To illustrate the power of this method we present results for the six-dimensional Hilbert space constituted by a qubit–qutrit system, which could be realized e.g. by the 14N nuclear spin-1 and two electronic spin states of a nitrogen-vacancy center in diamond. Measurements of the qubit subsystem are expressed by projectors of rank three, i.e. projectors on half-dimensional subspaces. For systems consisting only of qubits, it was shown analytically that a set of projectors on half-dimensional subspaces can be arranged in an informationally optimal fashion for QST, thus forming so-called mutually unbiased subspaces. Our method goes beyond qubits-only systems and we find that in dimension six such a set of mutually-unbiased subspaces can be approximated with a deviation irrelevant for practical applications.

Highlights

  • URL: http://nbn-resolving.de/urn:nbn:de:bsz:352-2-1vrrkulty6wx88There has been a strong interest in quantum computing since the publication of Shor’s algorithm [1] for prime factorization

  • We present a framework that formulates the quest for the most efficient quantum state tomography (QST) measurement set as an optimization problem which can be solved numerically, where the optimization goal is the maximization of the information gain

  • The measurements and computations which allow the estimation of a quantum state are called quantum state tomography (QST) [9]

Read more

Summary

Introduction

URL: http://nbn-resolving.de/urn:nbn:de:bsz:352-2-1vrrkulty6wx88There has been a strong interest in quantum computing since the publication of Shor’s algorithm [1] for prime factorization. Any physical system which is supposed to function as a building block of a quantum computer would require tests of its functionality. The measurements and computations which allow the estimation of a quantum state are called quantum state tomography (QST) [9]. QST is a central tool for verifying and debugging a quantum device and can be helpful for the process of implementation of a quantum computer in a physical system. It allows for checking of the initialization of the quantum device and—as a building block of quantum process tomography— the quantum gates

Objectives
Methods
Conclusion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.