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Corrigendum: Quantum state estimation with nuisance parameters (2020 J. Phys. A: Math. Theor.53 453001)

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Published 11 March 2024 © 2024 IOP Publishing Ltd
, , Citation Jun Suzuki et al 2024 J. Phys. A: Math. Theor. 57 129501 DOI 10.1088/1751-8121/ad2f10

This is a correction for 2020 J. Phys. A: Math. Theor. 53 453001

1751-8121/57/12/129501

Abstract

This is a correction for Suzuki et al (2020 J. Phys. A: Math. Gen.53 453001).

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We have found the two theorems (theorems 5.2 and 5.3) in section 5 appeared incorrectly. In particular, equations (112) and (114) were not correct.

Firstly, theorem 5.2 should state:

Theorem 5.2. Given a d-parameter regular model ${\cal M}$, for each d-dimensional (column) vector ${\boldsymbol{v}}\in{\mathbb{R}}^d$, the infimum of the MSE matrix in the direction of v is

Equation (112)

where $J_{\boldsymbol{\theta}}^{\mathrm{S}}$ is the SLD quantum Fisher information matrix. An optimal measurement is given by a projection measurement about the linear combination of the SLD operators:

Equation (113)

Secondly, theorem 5.3 should state:

Theorem 5.3. Given a d-parameter regular model ${\cal M}$, suppose that we are interested in estimating the parameter θ1 in the presence of the nuisance parameters $\boldsymbol{\theta}_{\mathrm{N}} = (\theta_2,\dots,\theta_d)$. The achievable lower bound for the MSE about the parameter of interest $V_{\boldsymbol{\theta};\mathrm{I}}[\hat{\Pi}_{\mathrm{I}}]$ is given by

Equation (114)

where the minimization is taken over all locally unbiased estimators $\hat{\Pi}_{\mathrm{I}}$ for the parameter of interest at θ , $J_{\boldsymbol{\theta}}^{\mathrm{S};1,1}$ is the (1, 1)th element of the inverse SLD matrix, and $J^{\mathrm{S}}_{\boldsymbol{\theta}}({\mathrm{I}}|{\mathrm{N}})$ is the partial SLD Fisher information (85). An optimal measurement is given by a projection measurement about the operator:

Equation (115)

10.1088/1751-8121/ad2f10