Optimizing the Choice of Spin-Squeezed States for Detecting and Characterizing Quantum Processes

Quantum metrology uses quantum states with no classical counterpart to measure a physical quantity with extraordinary sensitivity or precision. Most such schemes characterize a dynamical process by probing it with a specially designed quantum state. The success of such a scheme usually relies on the...

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Main Authors: Lee A. Rozema, Dylan H. Mahler, Robin Blume-Kohout, Aephraim M. Steinberg
Format: Article
Language:English
Published: American Physical Society 2014-11-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.4.041025
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spelling doaj-547fe2242c26436c95030bceb2145dae2020-11-24T23:32:22ZengAmerican Physical SocietyPhysical Review X2160-33082014-11-014404102510.1103/PhysRevX.4.041025Optimizing the Choice of Spin-Squeezed States for Detecting and Characterizing Quantum ProcessesLee A. RozemaDylan H. MahlerRobin Blume-KohoutAephraim M. SteinbergQuantum metrology uses quantum states with no classical counterpart to measure a physical quantity with extraordinary sensitivity or precision. Most such schemes characterize a dynamical process by probing it with a specially designed quantum state. The success of such a scheme usually relies on the process belonging to a particular one-parameter family. If this assumption is violated, or if the goal is to measure more than one parameter, a different quantum state may perform better. In the most extreme case, we know nothing about the process and wish to learn everything. This requires quantum process tomography, which demands an informationally complete set of probe states. It is very convenient if this set is group covariant—i.e., each element is generated by applying an element of the quantum system’s natural symmetry group to a single fixed fiducial state. In this paper, we consider metrology with 2-photon (“biphoton”) states and report experimental studies of different states’ sensitivity to small, unknown collective SU(2) rotations [“SU(2) jitter”]. Maximally entangled N00N states are the most sensitive detectors of such a rotation, yet they are also among the worst at fully characterizing an a priori unknown process. We identify (and confirm experimentally) the best SU(2)-covariant set for process tomography; these states are all less entangled than the N00N state, and are characterized by the fact that they form a 2-design.http://doi.org/10.1103/PhysRevX.4.041025
collection DOAJ
language English
format Article
sources DOAJ
author Lee A. Rozema
Dylan H. Mahler
Robin Blume-Kohout
Aephraim M. Steinberg
spellingShingle Lee A. Rozema
Dylan H. Mahler
Robin Blume-Kohout
Aephraim M. Steinberg
Optimizing the Choice of Spin-Squeezed States for Detecting and Characterizing Quantum Processes
Physical Review X
author_facet Lee A. Rozema
Dylan H. Mahler
Robin Blume-Kohout
Aephraim M. Steinberg
author_sort Lee A. Rozema
title Optimizing the Choice of Spin-Squeezed States for Detecting and Characterizing Quantum Processes
title_short Optimizing the Choice of Spin-Squeezed States for Detecting and Characterizing Quantum Processes
title_full Optimizing the Choice of Spin-Squeezed States for Detecting and Characterizing Quantum Processes
title_fullStr Optimizing the Choice of Spin-Squeezed States for Detecting and Characterizing Quantum Processes
title_full_unstemmed Optimizing the Choice of Spin-Squeezed States for Detecting and Characterizing Quantum Processes
title_sort optimizing the choice of spin-squeezed states for detecting and characterizing quantum processes
publisher American Physical Society
series Physical Review X
issn 2160-3308
publishDate 2014-11-01
description Quantum metrology uses quantum states with no classical counterpart to measure a physical quantity with extraordinary sensitivity or precision. Most such schemes characterize a dynamical process by probing it with a specially designed quantum state. The success of such a scheme usually relies on the process belonging to a particular one-parameter family. If this assumption is violated, or if the goal is to measure more than one parameter, a different quantum state may perform better. In the most extreme case, we know nothing about the process and wish to learn everything. This requires quantum process tomography, which demands an informationally complete set of probe states. It is very convenient if this set is group covariant—i.e., each element is generated by applying an element of the quantum system’s natural symmetry group to a single fixed fiducial state. In this paper, we consider metrology with 2-photon (“biphoton”) states and report experimental studies of different states’ sensitivity to small, unknown collective SU(2) rotations [“SU(2) jitter”]. Maximally entangled N00N states are the most sensitive detectors of such a rotation, yet they are also among the worst at fully characterizing an a priori unknown process. We identify (and confirm experimentally) the best SU(2)-covariant set for process tomography; these states are all less entangled than the N00N state, and are characterized by the fact that they form a 2-design.
url http://doi.org/10.1103/PhysRevX.4.041025
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