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This paper presents a novel numerical framework for simulating real-time dynamics in non-Hermitian quantum many-body systems using biorthogonal time-dependent variational principles. By employing matrix-free scaled Taylor actions, the method efficiently handles coupled left and right matrix-product states without storing dense matrices or Krylov bases. The approach successfully resolves dynamical quantum phase transitions in interacting long-range Ising chains, demonstrating how weak imaginary fields can shift critical times while addressing truncation-induced singularities.
Biorthogonal Time-Dependent Variational Principle for Non-Hermitian Systems
arXiv:2609.15099v1 Announce Type: new Abstract: We develop a biorthogonal time-dependent variational principle for real-time dynamics of non-Hermitian quantum many-body systems. Independent left and right matrix-product states obey coupled bivariational tangent-space equations whose cross-Gram matrix defines an oblique projection. A matrix-free scaled Taylor action propagates the resulting non-normal local generators without assembling dense matrices or storing a Krylov basis. We distinguish the fully coupled algorithm, which solves the cross-pairing problem and truncates the two bond bases jointly, from an efficient independently propagated approximation used for large systems. Independent truncation can make the retained left-right pairing nearly singular; overlap drift and the smallest singular value of the bond cross matrix expose this failure, while coupled truncation substantially delays it. Exact benchmarks and convergence tests validate the method. Applied to an interacting long-range non-Hermitian Ising chain, it resolves a biorthogonal dynamical quantum phase transition and shows that a weak imaginary field shifts the leading critical time from $t^{\ast}|J|=1.84$ to $1.04$.
Abstract:We develop a biorthogonal time-dependent variational principle for real-time dynamics of non-Hermitian quantum many-body systems. Independent left and right matrix-product states obey coupled bivariational tangent-space equations whose cross-Gram matrix defines an oblique projection. A matrix-free scaled Taylor action propagates the resulting non-normal local generators without assembling dense matrices or storing a Krylov basis. We distinguish the fully coupled algorithm, which solves the cross-pairing problem and truncates the two bond bases jointly, from an efficient independently propagated approximation used for large systems. Independent truncation can make the retained left-right pairing nearly singular; overlap drift and the smallest singular value of the bond cross matrix expose this failure, while coupled truncation substantially delays it. Exact benchmarks and convergence tests validate the method. Applied to an interacting long-range non-Hermitian Ising chain, it resolves a biorthogonal dynamical quantum phase transition and shows that a weak imaginary field shifts the leading critical time from $t^{\ast}|J|=1.84$ to $1.04$.
arXiv:2609.15099 [quant-ph]
(or arXiv:2609.15099v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2609.15099 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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