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    Metric structures characterized by norm properties in non-Hermitian systems

    Xin Wang1, Hao-Di Liu2,*, and Libin Fu1,†

    • *Contact author: liuhd100@nenu.edu.cn
    • †Contact author: lbfu@gscaep.ac.cn

    Phys. Rev. A 114, 052201 – Published 2 November, 2026

    DOI: https://doi.org/10.1103/6rg6-2n55

    Abstract

    For non-Hermitian quantum systems, metric operators provide a way to define the corresponding inner-product structures. In the entirely real-spectrum regime, a positive-definite metric η can be introduced such that the Hamiltonian is η-self-adjoint with respect to the corresponding inner product. In the complex-spectrum regime, different metric constructions can be characterized by their associated norm properties. For finite-dimensional non-Hermitian systems with a complete energy eigenbasis, we compare three representative metrics, namely, the cross-inner-product metric Υ1, the dynamical metric Υ2(t), and the pseudo-Hermitian metric Υ3, and analyze their relationships and differences. For time-independent Hamiltonians, the Υ1 norm obeys a balance equation governed by the imaginary parts of the eigenvalues, with its long-time behavior dominated by the largest imaginary part among contributions with nonzero initial weights. In contrast, Υ2(t) preserves the norm through its time dependence, while Υ3 remains norm-preserving but becomes indefinite in the complex-spectrum regime. For an entirely real spectrum, all three metrics coincide under the same normalization convention when Υ2(t0)=Υ1. At exceptional points, the energy eigenbasis is incomplete and Υ1 is singular and positive semidefinite, whereas a positive-definite Υ2(t) can be obtained from another complete initial basis, and a Hermitian invertible Υ3 can still be obtained from its defining equation. For time-dependent Hamiltonians, the Υ1(t) norm equation acquires a geometric contribution from the evolving biorthogonal basis, while imposing dynamical compatibility on Υ3(t) makes it coincide with Υ2(t) for the same initial metric. The corresponding exceptional-point properties are also discussed. A concrete model illustrates these distinctions.

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