2020
DOI: 10.22331/q-2020-07-02-288
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Optimal probes and error-correction schemes in multi-parameter quantum metrology

Abstract: We derive a necessary and sufficient condition for the possibility of achieving the Heisenberg scaling in general adaptive multi-parameter estimation schemes in presence of Markovian noise. In situations where the Heisenberg scaling is achievable, we provide a semidefinite program to identify the optimal quantum error correcting (QEC) protocol that yields the best estimation precision. We overcome the technical challenges associated with potential incompatibility of the measurement optimally extracting… Show more

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Cited by 49 publications
(51 citation statements)
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“…Recent work shows that it is possible to measure H at the Heisenberg limit using an error-correcting code if H cannot be expressed as a linear combination of correctable noise operators [100][101][102][103][104]. But if the physical charge T A is a sum of local charges, the Eastin-Knill theorem poses a challenge to the application of error-correcting techniques; namely, error correction prevents probe states from evolving, obscuring the signal.…”
Section: Discussionmentioning
confidence: 99%
“…Recent work shows that it is possible to measure H at the Heisenberg limit using an error-correcting code if H cannot be expressed as a linear combination of correctable noise operators [100][101][102][103][104]. But if the physical charge T A is a sum of local charges, the Eastin-Knill theorem poses a challenge to the application of error-correcting techniques; namely, error correction prevents probe states from evolving, obscuring the signal.…”
Section: Discussionmentioning
confidence: 99%
“…Beyond these direct applications, it provides a crucial fundamental milestone of experimental witnessing of intrinsic properties of highly nonclassical states applicable to a broad spectrum of modern applications of quantum-enhanced control and measurement of mechanical motion including the optical frequency metrology [38,39], quantum error correction [8,[15][16][17], tests of quantum thermodynamical phenomena [40,41], or gravitational wave detection [42]. Together with the recent demonstration of viable preparation of states with properties suggesting their proximity to number states with up to |n ∼ 100 on the same experimental platform [9], presented approach will allow for optimization and comparison of these quantum states across different sensing scenarios with a clearly identifiable fundamental and application relevance [43,44]. We foresee a further enhancement of the presented states approaching idealized Fock states by operating the experiment at a much higher trapping frequencies, which will allow for speed up of the state preparation procedure and minimization of the corresponding thermalization process duration.…”
Section: Discussionmentioning
confidence: 99%
“…To regain the quantum advantage, one needs to combine quantum error correction with quantum sensing. Indeed, if the noise acts sufficiently different than the signal, we can retain the Heisenberg scaling by using a metrological code [57,58]. For certain noise models, scalings between standard and Heisenberg scaling can be achieved [59].…”
Section: Quantifying Sensing Performance the Classicalmentioning
confidence: 99%