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This paper introduces a symmetry-projection framework for multiparameter quantum sensing, demonstrating how specific symmetries can eliminate cross-sector elements in the quantum Fisher information matrix to simplify uncertainty quantification. The authors show that this approach enables direct certification of sensitivity via spin fluctuations and allows mixed states to achieve Heisenberg-limited precision over broad time windows in dissipative systems.
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Symmetry-Projected Compatible Multiparameter Quantum Sensing

arXiv2 min read

arXiv:2608.01831v1 Announce Type: new Abstract: We establish a general symmetry-projection framework for multiparameter quantum sensing. Decomposing encoding generators into subspace-preserving and subspace-changing components relative to a symmetry sector identically eliminates all cross-sector elements of the quantum Fisher information matrix (QFIM) and the mean symmetric logarithmic derivative (SLD) commutator matrix. When projected subspace-changing generators act as a scalar within the occupied subspace, the corresponding QFIM block reduces to four times the symmetrized covariance matrix, regardless of probe state purity. For parity-protected collective $\mathrm{SU}(2)$ spin systems, this renders the transverse QFIM directly certifiable via spin fluctuations, with the optimal axis aligned with the anti-squeezed quadrature. Applied to a dissipative one-axis-twisting system, our framework reveals that highly mixed transient states can exhibit nearly balanced, Heisenberg-scaled QFIM components for transverse--longitudinal parameter pairs $(\theta_y,\theta_z)$ over a broad time window. Furthermore, while the steady state retains an isotropic transverse QFIM scaling as $N^2/3$, weak compatibility for transverse parameter pairs $(\theta_x,\theta_y)$ exhibits a sharp parity dependence---failing for odd $N$ but restored for even $N$. The resulting symmetry protection eliminates the Uhlmann curvature for transverse--longitudinal pairs, enabling simultaneous saturation of the multi-parameter quantum Cram\'{e}r-Rao bound in the asymptotic limit.

Abstract:We establish a general symmetry-projection framework for multiparameter quantum sensing. Decomposing encoding generators into subspace-preserving and subspace-changing components relative to a symmetry sector identically eliminates all cross-sector elements of the quantum Fisher information matrix (QFIM) and the mean symmetric logarithmic derivative (SLD) commutator matrix. When projected subspace-changing generators act as a scalar within the occupied subspace, the corresponding QFIM block reduces to four times the symmetrized covariance matrix, regardless of probe state purity. For parity-protected collective $\mathrm{SU}(2)$ spin systems, this renders the transverse QFIM directly certifiable via spin fluctuations, with the optimal axis aligned with the anti-squeezed quadrature. Applied to a dissipative one-axis-twisting system, our framework reveals that highly mixed transient states can exhibit nearly balanced, Heisenberg-scaled QFIM components for transverse--longitudinal parameter pairs $(\theta_y,\theta_z)$ over a broad time window. Furthermore, while the steady state retains an isotropic transverse QFIM scaling as $N^2/3$, weak compatibility for transverse parameter pairs $(\theta_x,\theta_y)$ exhibits a sharp parity dependence---failing for odd $N$ but restored for even $N$. The resulting symmetry protection eliminates the Uhlmann curvature for transverse--longitudinal pairs, enabling simultaneous saturation of the multi-parameter quantum Cramér-Rao bound in the asymptotic limit.

6.2 pages, 1 figures

Quantum Physics (quant-ph); Atomic Physics (physics.atom-ph); Optics (physics.optics)

arXiv:2608.01831 [quant-ph]

(or arXiv:2608.01831v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2608.01831 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 289 words

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