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arXiv:2607.10118

Hamiltonian Conditions for Dark Modes in Multimode Bosonic Systems

Zuxin Wu, Shengshi Pang

quant-phphysics.opticsSubmitted Jul 11, 2026• Announced Jul 14, 2026• 0 citations
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Abstract

Dark modes arise when destructive interference prevents selected bosonic degrees of freedom from coupling to environmental channels. We formulate a Hamiltonian criterion for identifying such modes in multimode bosonic systems by separating two requirements: the candidate mode must be invisible to the direct system--environment coupling, and its generated operator space must remain invariant under the intrinsic system dynamics. For linear environment coupling and quadratic system Hamiltonians, the criterion is reduced to the the familiar null-space and invariant-subspace conditions of passive linear dark-mode theory. We then extend the analysis to nonlinear scenarios. For a two-photon conversion channel coupled to an auxiliary environmental mode, interference among nonlinear conversion pathways can reduce the environment coupling to a single collective two-photon channel, leaving a complementary bosonic mode decoupled from the environment. We show that preserving this mode under nonlinear intrinsic dynamics generally requires more than conventional Kerr-type quartic interactions: correlated four-boson conversion processes are needed to cancel mixed nonlinear conversion between the dark and environment-coupled collective modes. Finally, we show that the Bogoliubov dark mode of a parametrically driven optomechanical satisfies the same Hamiltonian criterion through an active canonical transformation. These results provide a unified Hamiltonian framework for identifying and engineering dark modes in linear, nonlinear, and driven bosonic systems.

Comments
17 pages, 2 figures. Submitted to Physical Review A

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We propose and prove two theorems for determining the number of dark modes in linear two-component quantum networks composed of two types of bosonic modes. This is achieved by diagonalizing the two sub-networks of the same type of modes, mapping the networks to either a standard or a thick arrowhead matrix, and analyzing the linear dependence and independence between the column vectors associated with degenerate normal modes in the coupling matrix. We confirm the two theorems by checking the simultaneous ground-state cooling of the mechanical modes in linearized optomechanical networks. These results also work for linear fermionic networks and other networks described by quadratic coupled-mode Hamiltonian. The present method can be extended to study the dark-state effect in driven atom systems and to construct large decoherence-free subspaces for processing quantum information. This work will initiate the studies on dynamical, transport, and statistical properties of linear networks with decoupled subspaces.
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Abstract Determining dark modes in quadratic bosonic networks is both fundamental and imperative, since the dark modes are critical to coherent network manipulation and quantum resource transfer, and such networks are applicable to wide parameter regimes and various physical areas. Here, we develop a symplectic singular value decomposition (SSVD) method for identifying the number and form of the dark modes in quadratic bosonic networks. This method maps the emergence of dark modes onto a computationally tractable symplectic null-space problem, enabling their systematic identification in large-scale quadratic bosonic networks.We adopt the SSVD method to study both the collective cooling of multiple mechanical modes and optomechanical entanglement generation in linearized optomechanical networks. We find that the appearance of the dark modes suppresses the cooling performance and entanglement generation. Our work paves the way for engineering dark modes in quadratic bosonic networks, and the SSVD method has wide applicability in quantum physics, quantum information science, and many-body physics.
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