Time-Dependent Pseudo-Hermitian Hamiltonians and a Hidden Geometric Aspect of Quantum Mechanics

Abstract

A non-Hermitian operator $H$ defined in a Hilbert space with inner product $⟨\cdot |\cdot ⟩$ may serve as the Hamiltonian for a unitary quantum system, if it is $\eta$-pseudo-Hermitian for a metric operator (positive-definite automorphism) $\eta$. The latter defines the inner product $⟨\cdot |\eta \cdot ⟩$ of the physical Hilbert space ${\mathcal{H}}_{\eta }$ of the system. For situations where some of the eigenstates of $H$ depend on time, $\eta$ becomes time-dependent. Therefore the system has a non-stationary Hilbert space. Such quantum systems, which are also encountered in the study of quantum mechanics in cosmological backgrounds, suffer from a conflict between the unitarity of time evolution and the unobservability of the Hamiltonian. Their proper treatment requires a geometric framework which clarifies the notion of the energy observable and leads to a geometric extension of quantum mechanics (GEQM). We provide a general introduction to the subject, review some of the recent developments, offer a straightforward description of the Heisenberg-picture formulation of the dynamics for quantum systems having a time-dependent Hilbert space, and outline the Heisenberg-picture formulation of dynamics in GEQM.

28 pages, 1 figure

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Cited by in corpus (8)

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• Anomalous dynamical response of non-Hermitian topological phases
• Real energies and Berry phases in all PT-regimes in time-dependent non-Hermitian theories
• Non-Hermitian Quantum Quenches in Holography
• Linear Response for pseudo-Hermitian Hamiltonian Systems: Application to PT-Symmetric Qubits
• Consistent treatment of quantum systems with a time-dependent Hilbert space
• Hilbert space representation for quasi-Hermitian position-deformed Heisenberg algebra and Path integral formulation