2013
DOI: 10.1103/physrevlett.110.240405
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Matrix Product States for Quantum Metrology

Abstract: We demonstrate that the optimal states in lossy quantum interferometry may be efficiently simulated using low rank matrix product states. We argue that this should be expected in all realistic quantum metrological protocols with uncorrelated noise and is related to the elusive nature of the Heisenberg precision scaling in the asymptotic limit of large number of probes.

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Cited by 41 publications
(37 citation statements)
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“…In case channels L x are noisy, the QFI at the output for optimally entangled input probes generically scales linearly with k and the quantum enhancement amount to a constant factor improvement [38]. Moreover, as argued in [62,64] one can achieve almost optimal performance utilizing states where k probes are divided into groups of g particles where entanglement is present only among the particles belonging to the same group. In such a scenario, one can approximate the input state as a product state of large number of groups, number of which will tend to infinity while their size will remain constant when  ¥ k .…”
Section: Strong Estimation Regimementioning
confidence: 99%
“…In case channels L x are noisy, the QFI at the output for optimally entangled input probes generically scales linearly with k and the quantum enhancement amount to a constant factor improvement [38]. Moreover, as argued in [62,64] one can achieve almost optimal performance utilizing states where k probes are divided into groups of g particles where entanglement is present only among the particles belonging to the same group. In such a scenario, one can approximate the input state as a product state of large number of groups, number of which will tend to infinity while their size will remain constant when  ¥ k .…”
Section: Strong Estimation Regimementioning
confidence: 99%
“…We overcome the problem of mixed states by considering the combined state of the system and output. This is a pure quantum state-actually a matrix product state (MPS) [13,14,16,17]-which encodes the state of the system as well as the record of emissions for the whole observation time. This allows us to find the best estimation precision using the system-output state as a resource.…”
Section: Introductionmentioning
confidence: 99%
“…In such circumstance, for the asymptotic regime where a large number N of qubits are available, an efficient strategy, as also considered for instance in Ref. [36], would be to group the N qubits into independent blocks of N opt optimally entangled qubits. For such strategy with entanglement, the asymptotic regime of large N would be characterized, in terms of Fisher information, by an efficiency growing linearly with N, yet with a level strictly superior to the efficiency of the strategy using the optimal separable probe (which also grows linearly with N).…”
Section: Optimum At Partial Entanglementmentioning
confidence: 99%