Learning Arbitrary Lindbladians with Quantum Error Correction
Abstract
We study ansatz-free Lindbladian learning, the problem of reconstructing the generator of an open quantum system without prior knowledge of its Hamiltonian or dissipator structures. This problem exhibits two fundamental precision limits. Hamiltonian components not obscured by dissipation are Heisenberg-limited, while full Lindbladian reconstruction is subject to the quadratically worse standard quantum limit. This creates an apparent algorithmic impasse: achieving the Heisenberg-limited Hamiltonian learning requires suppressing unknown dissipation, which seemingly demands prior reconstruction of the noise and thereby incurs the standard-quantum-limit cost. In this work, we resolve this obstruction by giving an algorithm that learns the Hamiltonian disjoint from dissipator (HDD) at the Heisenberg limit without prior knowledge of either the Hamiltonian or dissipator supports. Our main technical ingredient is a randomized recursive stabilizer-code construction that progressively identifies and suppresses the dominant dissipative terms without reconstructing the full dissipator. Building on this framework, we also introduce an efficient end-to-end algorithm that learns the entire sparse Lindbladian at the standard quantum limit. Finally, we prove that in the ansatz-free setting, the HDD terms constitute the maximal set of Hamiltonian coefficients uniformly learnable at the Heisenberg limit. We show that every term outside HDD is fundamentally standard-quantum limited, extending prior no-go results to the ansatz-free setting. Together, our protocols provide a scalable framework for characterizing open quantum systems, with quantum error correction serving as a key learning primitive.
Related
- Learning Logical Operations for Arbitrary Quantum Error Correction Codes
- Learning Arbitrary Lindbladians from Time Evolution
- Bosonic quantum error correction with microwave cavities for quantum repeaters
- Error-Correction Transitions in Finite-Depth Quantum Channels
- Quantum Error Correction and the Limits of Quantum Metrology
BibTeX
@misc{romanov2026learning,
title = {{Learning Arbitrary Lindbladians with Quantum Error Correction}},
author = {Nikita Romanov and Petr Ivashkov and Weiyuan Gong and Ishaan Kannan and Andi Gu and Hong-Ye Hu and Susanne F. Yelin},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2606.18188},
eprint = {2606.18188},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2606.18188},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Learning Arbitrary Lindbladians with Quantum Error Correction
AU - Nikita Romanov
AU - Petr Ivashkov
AU - Weiyuan Gong
AU - Ishaan Kannan
AU - Andi Gu
AU - Hong-Ye Hu
AU - Susanne F. Yelin
PY - 2026
DA - 2026/10/05
PB - arXiv
DO - 10.48550/arxiv.2606.18188
UR - https://arxiv.org/abs/2606.18188
AB - We study ansatz-free Lindbladian learning, the problem of reconstructing the generator of an open quantum system without prior knowledge of its Hamiltonian or dissipator structures. This problem exhibits two fundamental precision limits. Hamiltonian components not obscured by dissipation are Heisenberg-limited, while full Lindbladian reconstruction is subject to the quadratically worse standard quantum limit. This creates an apparent algorithmic impasse: achieving the Heisenberg-limited Hamiltonian learning requires suppressing unknown dissipation, which seemingly demands prior reconstruction of the noise and thereby incurs the standard-quantum-limit cost. In this work, we resolve this obstruction by giving an algorithm that learns the Hamiltonian disjoint from dissipator (HDD) at the Heisenberg limit without prior knowledge of either the Hamiltonian or dissipator supports. Our main technical ingredient is a randomized recursive stabilizer-code construction that progressively identifies and suppresses the dominant dissipative terms without reconstructing the full dissipator. Building on this framework, we also introduce an efficient end-to-end algorithm that learns the entire sparse Lindbladian at the standard quantum limit. Finally, we prove that in the ansatz-free setting, the HDD terms constitute the maximal set of Hamiltonian coefficients uniformly learnable at the Heisenberg limit. We show that every term outside HDD is fundamentally standard-quantum limited, extending prior no-go results to the ansatz-free setting. Together, our protocols provide a scalable framework for characterizing open quantum systems, with quantum error correction serving as a key learning primitive.
ER -