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Phys. Rev. A 80, 052114 (2009) [22 pages]

How to perform the most accurate possible phase measurements

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D. W. Berry1,2, B. L. Higgins3, S. D. Bartlett4, M. W. Mitchell5, G. J. Pryde3,*, and H. M. Wiseman3,†
1Institute for Quantum Computing, University of Waterloo, Waterloo, Ontario, Canada N2L 3G1
2Centre for Quantum Computer Technology, Department of Physics, Macquarie University, Sydney 2109, Australia
3Centre for Quantum Computer Technology, Centre for Quantum Dynamics, Griffith University, Brisbane 4111, Australia
4School of Physics, University of Sydney, Sydney 2006, Australia
5ICFO-Institut de Ciencies Fotoniques, Mediterranean Technology Park, 08860 Castelldefels (Barcelona), Spain

Received 30 June 2009; published 23 November 2009

We present the theory of how to achieve phase measurements with the minimum possible variance in ways that are readily implementable with current experimental techniques. Measurements whose statistics have high-frequency fringes, such as those obtained from maximally path-entangled (|N,0⟩+|0,N⟩)/√2 (“NOON”) states, have commensurately high information yield (as quantified by the Fisher information). However, this information is also highly ambiguous because it does not distinguish between phases at the same point on different fringes. We provide schemes to eliminate this phase ambiguity in a highly efficient way, providing phase estimates with uncertainty that is within a small constant factor of the Heisenberg limit, the minimum allowed by the laws of quantum mechanics. These techniques apply to NOON state and multipass interferometry, as well as phase measurements in quantum computing. We have reported the experimental implementation of some of these schemes with multipass interferometry elsewhere. Here, we present the theoretical foundation and also present some additional experimental results. There are three key innovations to the theory in this paper. First, we examine the intrinsic phase properties of the sequence of states (in multiple time modes) via the equivalent two-mode state. Second, we identify the key feature of the equivalent state that enables the optimal scaling of the intrinsic phase uncertainty to be obtained. This enables us to identify appropriate combinations of states to use. The remaining difficulty is that the ideal phase measurements to achieve this intrinsic phase uncertainty are often not physically realizable. The third innovation is to solve this problem by using realizable measurements that closely approximate the optimal measurements, enabling the optimal scaling to be preserved. We consider both adaptive and nonadaptive measurement schemes.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevA.80.052114
DOI:
10.1103/PhysRevA.80.052114
PACS:
03.65.Ta, 42.50.St, 03.67.−a

*g.pryde@griffith.edu.au

h.wiseman@griffith.edu.au