Neural quantum states for non-Markovian open quantum dynamics in bosonic environments
5 affiliations
- 1State Key Laboratory of Porous Materials for Separation and Conversion & MOE Key Laboratory of Computational Physical Sciences & Department of Chemistry
- 2Fudan University
- 3Hefei National Research Center for Physical Sciences at the Microscale
- 4University of Science and Technology of China
- 5Hefei National Laboratory
Abstract
Condensed-phase quantum dynamics are strongly shaped by vibrational, solvent, and protein environments, yet their nonperturbative, non-Markovian description requires a rapidly growing high-dimensional representation as environmental complexity increases. Here, we extend neural quantum states (NQS) to the dissipaton-embedded quantum master equation (DQME) for bosonic environments using a complex-valued restricted Boltzmann machine adapted to nonbinary bosonic occupations. An explicit filtering scheme further concentrates the neural representation on dynamically relevant dissipaton configurations. The resulting NQS-DQME approach reproduces representative quantum dissipative dynamics while effectively compressing the reduced density tensor (RDT). For an anharmonic model of condensed-phase hydrogen transfer, the method also reproduces weak-coupling tunneling dynamics. At stronger system-bath coupling, however, errors become localized in a small subset of RDT elements, showing that a small global variational residual does not necessarily ensure accurate chemically relevant observables. This limitation identifies observable-level error control as a key challenge for reliable long-time NQS propagation.
Related
- Excited-State Intramolecular Proton Transfer Dynamics with Neural Network Potentials and Nuclear Quantum Effects
- Reaction dynamics in non-Markovian systems with non-monotonically decaying memory
- A General Non-Markovian Electronic Friction and Langevin Dynamics Framework for Nonequilibrium Systems
- UGME: A python package for non-Markovian protein folding dynamics
- Improving the Stability of the Hierarchical Equations of Motion for Open Quantum Systems with Strong Coupling to Structured Bosonic Baths
BibTeX
@misc{zhu2026neural,
title = {{Neural quantum states for non-Markovian open quantum dynamics in bosonic environments}},
author = {Qingdong Zhu and Long Cao and Liwei Ge and Zhiqian Huang and Igor Ying Zhang and Xin Xu and Xiao Zheng},
howpublished = {ChemRxiv},
year = {2026},
month = oct,
doi = {10.26434/chemrxiv.15011173/v1},
url = {https://chemrxiv.org/doi/full/10.26434/chemrxiv.15011173/v1},
note = {CC BY},
}
RIS
TY - UNPB
TI - Neural quantum states for non-Markovian open quantum dynamics in bosonic environments
AU - Qingdong Zhu
AU - Long Cao
AU - Liwei Ge
AU - Zhiqian Huang
AU - Igor Ying Zhang
AU - Xin Xu
AU - Xiao Zheng
PY - 2026
DA - 2026/10/28
PB - ChemRxiv
DO - 10.26434/chemrxiv.15011173/v1
UR - https://chemrxiv.org/doi/full/10.26434/chemrxiv.15011173/v1
AB - Condensed-phase quantum dynamics are strongly shaped by vibrational, solvent, and protein environments, yet their nonperturbative, non-Markovian description requires a rapidly growing high-dimensional representation as environmental complexity increases. Here, we extend neural quantum states (NQS) to the dissipaton-embedded quantum master equation (DQME) for bosonic environments using a complex-valued restricted Boltzmann machine adapted to nonbinary bosonic occupations. An explicit filtering scheme further concentrates the neural representation on dynamically relevant dissipaton configurations. The resulting NQS-DQME approach reproduces representative quantum dissipative dynamics while effectively compressing the reduced density tensor (RDT). For an anharmonic model of condensed-phase hydrogen transfer, the method also reproduces weak-coupling tunneling dynamics. At stronger system-bath coupling, however, errors become localized in a small subset of RDT elements, showing that a small global variational residual does not necessarily ensure accurate chemically relevant observables. This limitation identifies observable-level error control as a key challenge for reliable long-time NQS propagation.
ER -