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Simple expression for the quantum Fisher information matrix

Published 3 Jan 2018 in quant-ph and cond-mat.quant-gas | (1801.00945v2)

Abstract: Quantum Fisher information matrix (QFIM) is a cornerstone of modern quantum metrology and quantum information geometry. Apart from optimal estimation, it finds applications in description of quantum speed limits, quantum criticality, quantum phase transitions, coherence, entanglement, and irreversibility. We derive a surprisingly simple formula for this quantity, which, unlike previously known general expression, does not require diagonalization of the density matrix, and is provably at least as efficient. With a minor modification, this formula can be used to compute QFIM for any finite-dimensional density matrix. Because of its simplicity, it could also shed more light on the quantum information geometry in general.

Summary

  • The paper introduces a novel direct formula for QFIM computation, eliminating the need for density matrix diagonalization.
  • It employs vectorization and Kronecker products, using regularization and Cholesky decomposition to enhance computational efficiency.
  • The approach improves parameter estimation in quantum metrology by providing precise error bounds and streamlined calculations.

Simple Expression for the Quantum Fisher Information Matrix

Introduction

The focus of this paper is on deriving a simplified expression for the Quantum Fisher Information Matrix (QFIM), which is crucial in various domains of quantum mechanics, including quantum metrology and quantum information geometry. The primary result is a novel formula that bypasses the need for diagonalizing the density matrix—a traditional requirement that can be computationally intensive. This development holds promise for enhancing the efficiency of QFIM computations and broadening the understanding of its implications in quantum systems.

Quantum Fisher Information Matrix and Its Applications

The QFIM is foundational in quantum metrology, primarily due to its role in defining the quantum Cramér-Rao bound, a theoretical limit on the precision of parameter estimation in quantum systems. Diverse fields such as quantum speed limits, phase transitions, coherence, and entanglement employ QFIM. The attractiveness of the QFIM lies in its capacity to deliver quantitative insights into the sensitivity and fidelity of quantum state evolution under varying parameters.

New Formula for QFIM

Theoretical Contribution

The paper introduces a direct formula for calculating the QFIM without the necessity for matrix diagonalization:

Hij=2vec(i)(ρI+Iρ)1vec(j)H^{ij} = 2 \, \text{vec}(\partial_i)^\dagger \big( \rho \otimes I + I \otimes \rho \big)^{-1} \text{vec}(\partial_j)

This innovation hinges on vectorization and Kronecker products, simplifying operations on the density matrix ρ\rho. Not only does the new formula circumvent eigenvalue decompositions, but it maintains computational efficiency, even for non-invertible matrices through regularization techniques.

Implementation Insights

The practical implementation of this formula involves calculating the vectorized partial derivatives of the density matrix with respect to estimation parameters and handling matrix inversions that are efficiently manageable via decomposition methods like Cholesky when computational limits are strained. Such implementation allows for calculations in any chosen basis, facilitating flexibility and possibly reducing computational overhead.

Applications and Examples

Two key examples underscore the applicability of the derived formula. The first example explores simultaneous estimation of phase and noise within a quantum system, leveraging the simplified calculation method to illustrate fundamental principles such as error bounds in joint parameter estimation. The second example includes phase estimation using maximally entangled states, yielding significant insights into the errors and precision limits of practical quantum measurement setups.

Computational Advantage

The formula's ability to operate directly on the density matrix without dependency on eigenvectors provides a clear computational advantage. All traditional steps requiring manual diagonalization can be replaced by automated matrix operations, potentially streamlining simulations and theoretical predictions in quantum information studies.

Conclusion

The paper presents a significant step towards refining computational strategies in quantum mechanics by introducing a formula that simplifies the calculation of QFIM. This advancement offers substantial reduction in complexity, enabling broader application in quantum research and development across various technological domains. Further exploration into computational optimization techniques and their impact on quantum system design remains a promising venture following these findings.

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