Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:2410.18635 · Physical Review A

Path integral control of open quantum systems

Aarón Villanueva, Hilbert J. Kappen

Published Jun 9, 2026• 0 citations
arXivHTMLPDF

Abstract

We investigate open-loop quantum state preparation for a class of open quantum systems whose dynamics follow a Gorini-Kossakowski-Lindblad-Sudarshan (GKLS) master equation that admits a trajectory-based stochastic representation. The deterministic control objective is reformulated as a stochastic optimal control problem -- interpreting stochasticity as a methodological tool akin to stochastic Schrödinger equation unravelings -- which situates the problem within the path integral control framework. For the class of GKLS generators under consideration, this reformulation leads to an explicit expression for the optimal control as a weighted average over stochastic quantum trajectories, thereby eliminating the need for gradient evaluations. Building on this theoretical result, we derive a control update rule for piecewise-constant control pulses and demonstrate that adaptive importance sampling progressively enhances the control estimator during optimization, culminating in the algorithm we term Path integral Quantum Control (PiQC). We further introduce an annealed variant of PiQC, wherein a synthetic noise schedule gradually steers open-system trajectories toward closed-system dynamics, enabling high-fidelity unitary state preparation. Numerical studies on a dissipative single-qubit system and a multi-qubit Nuclear Magnetic Resonance model verify that PiQC yields precise open-loop controls and displays robustness to Hamiltonian perturbations. We propose PiQC as a trajectory-based alternative to gradient-based approaches, which might offer a viable solution in quantum control problems where gradient computation is infeasible or computationally demanding.

DOI
10.1103/kwxb-3jy1

Related papers

Gate-based path integral quantum control applied to quantum chemistry

Peyman Najafi, Aarón Villanueva, Hilbert J. Kappen

Abstract The Path integral Quantum Control (PiQC) algorithm was recently introduced as a new approach for computing optimal controls in continuous-time open and closed quantum systems. In this work, we adapt the PiQC algorithm to optimize parametrized quantum circuits and refer to this version of PiQC as the Gate-Based PiQC (GB-PiQC) algorithm. We apply GB-PiQC and the original continuous-time version of PiQC for ground state preparation of electronic structure problems, and benchmark them against the Variational Quantum Eigensolver, optimized using the standard Simultaneous Perturbation Stochastic Approximation (SPSA) optimizer, on a set of standard benchmark molecular Hamiltonians. For a fair comparison, we optimize the hyperparameters of the algorithms for each molecule. We find that both PiQC algorithms exhibit greater robustness than SPSA to variations in the target Hamiltonian induced by changes in interatomic distance, when hyperparameters for both methods are fixed at values tuned near equilibrium. Furthermore, PiQC algorithms also achieve superior performance compared to SPSA in most instances under this fixed-hyperparameter setting, particularly at stretched interatomic distances, where the Hartree–Fock solution becomes less accurate and its error grows relative to equilibrium.

Quantum Science and Technology•Oct 13, 2026•0 citations

Optimal Controls for Open Quantum Systems Using Stochastic Path Integrals

Wirawat Kokaew, Thiparat Chotibut, Areeya Chantasri

We propose a new optimal control protocol for quantum state preparation in the presence of environmental noises based on the Most Likely Path (MLP) approach. The standard method for dealing with unknown noises in open quantum systems is via Lindblad master equation, which describes the Mean Path (MP) of noisy quantum trajectories. However, the mean path does not always faithfully represent the ensemble of trajectories, especially when the trajectory distribution is multimodal. The most likely path of quantum trajectories is extracted from stochastic path integral formulation, constructed from the joint probability of quantum statetrajectories and the noises. We study a quantum control problem of a single-qubit state preparation, controlling the qubit from an arbitrary initial state to the desired target state in the presence of a dephasing noise, where the control is the Rabi oscillation. This approach yields the analytical solution for the optimal control protocol for the Rabi drive, which is not possible using the standard MP approach. We also investigate the benefits of optimal Rabi drive by looking at the distribution of final states in the Bloch sphere; we find that the distribution of final state is concentrated around the desired target state and does not spread out over the qubit.

•Jan 1, 2020•0 citations

On optimization of coherent and incoherent controls for two-level quantum systems

Oleg Vasilevich Morzhin, Alexander Nikolaevich Pechen

This paper considers some control problems for closed and open two-level quantum systems. The closed system's dynamics is governed by the Schrödinger equation with coherent control. The open system dynamics is governed by the Gorini-Kossakowski-Sudarshan-Lindblad master equation whose Hamiltonian depends on coherent control and superoperator of dissipation depends on incoherent control. For the closed system, we consider the problem of generation of the phase shift gate for some values of phases and final times for which we numerically show that zero coherent control, which is a stationary point of the objective functional, is not optimal; it gives an example of subtle point for practical solving quantum control problems. The two-stage method, which was developed in [48] for generic $N$-level open quantum systems for approximate generation of a given target density matrix, is modified here for the case of two-level systems. We modify the first ("incoherent") stage by numerically optimizing piecewise constant incoherent control instead of using constant incoherent control analytically computed using eigenvalues of the target density matrix. Exact analytical formulas are derived for the system state evolution, the objective functions and their gradients for the modified first stage. These formulas are then applied in the two-step gradient projection method. The numerical simulations show that the modified first stage duration can be significantly less than the unmodified first stage duration, but at the cost of performing optimization in the class of piecewise constant controls.

arXiv:2205.02521•Izvestiya Mathematics•Jan 1, 2023•8 citations

Path integral control in the complex plane

Aarón Villanueva

Path integral control is a stochastic optimal control framework that computes optimal policies as weighted averages over state trajectories. It was recently shown that, combined with stochastic quantum trajectories, the path integral control approach constitutes a promising alternative for quantum optimal control. In this work, we propose an extension of path integral control to the complex plane using circular complex Wiener processes. The change of measure is defined on the driving noise space under an exact control-noise matching condition, which also accommodates rank-deficient state diffusions. Applied to stochastic Schrödinger equations, the resulting formalism gives a compact treatment of paired non-Hermitian jump channels with unequal positive dissipation rates and yields cross-entropy-optimal feedback and open-loop control formulas.

quant-pharXiv:2610.34483•Oct 27, 2026•0 citations

On optimization of coherent and incoherent controls for two-level quantum systems

Oleg Vasilevich Morzhin, Alexander Nikolaevich Pechen

This article considers some control problems for closed and open two-level quantum systems. The closed system's dynamics is governed by the Schrödinger equation with coherent control. The open system's dynamics is governed by the Gorini-Kossakowski-Sudarshan-Lindblad master equation whose Hamiltonian depends on coherent control and superoperator of dissipation depends on incoherent control. For the closed system, we consider the problem for generation of the phase shift gate for some values of phases and final times for which we numerically show that zero coherent control, which is a stationary point of the objective functional, is not optimal; it gives an example of subtle point for practical solving quantum control problems. The two-stage method, which was developed in [A. Pechen, Phys. Rev. A., 84, 042106 (2011)] for generic $N$-level open quantum systems for approximate generation of a given target density matrix, is modified here for the case of two-level systems. We modify the first ("incoherent") stage by numerically optimizing piecewise constant incoherent control instead of using constant incoherent control analytically computed using eigenvalues of the target density matrix. Exact analytical formulas are derived for the system's state evolution, the objective functions and their gradients for the modified first stage. These formulas are then applied in the two-step gradient projection method. The numerical simulations show that the modified first stage's duration can be significantly less than the unmodified first stage's duration, but at the cost of performing optimization in the class of piecewise constant controls. Bibliography: 72 titles.

Известия Российской академии наук Серия математическая•Jan 1, 2023•0 citations

Quantum Annealing Complexity and Stochastic Quantum Control

Aarón Villanueva

This thesis investigates two central challenges for quantum computing: identifying when quantum annealing can offer a computational advantage, and developing effective methods to control realistic quantum systems. It establishes complexity bounds for an adiabatic algorithm for combinatorial optimization, showing a universal quadratic advantage while highlighting the practical difficulty of realizing the required schedule. It also introduces Path Integral Quantum Control, a trajectory-based framework for optimizing controls in open quantum systems, and develops a stochastic Hamiltonian description of continuous quantum measurement connected to double-bracket gradient flows. Together, these results advance the theoretical foundations of quantum optimization, open-system control, and measurement-based feedback

Radboud University Press eBooks•Sep 23, 2026•0 citations
We investigate open-loop quantum state preparation for a class of open quantum systems whose dynamics follow a Gorini-Kossakowski-Lindblad-Sudarshan (GKLS) master equation that admits a trajectory-based stochastic representation. The deterministic control objective is reformulated as a stochastic optimal control problem -- interpreting stochasticity as a methodological tool akin to stochastic Schrödinger equation unravelings -- which situates the problem within the path integral control framework. For the class of GKLS generators under consideration, this reformulation leads to an explicit expression for the optimal control as a weighted average over stochastic quantum trajectories, thereby eliminating the need for gradient evaluations. Building on this theoretical result, we derive a control update rule for piecewise-constant control pulses and demonstrate that adaptive importance sampling progressively enhances the control estimator during optimization, culminating in the algorithm we term Path integral Quantum Control (PiQC). We further introduce an annealed variant of PiQC, wherein a synthetic noise schedule gradually steers open-system trajectories toward closed-system dynamics, enabling high-fidelity unitary state preparation. Numerical studies on a dissipative single-qubit system and a multi-qubit Nuclear Magnetic Resonance model verify that PiQC yields precise open-loop controls and displays robustness to Hamiltonian perturbations. We propose PiQC as a trajectory-based alternative to gradient-based approaches, which might offer a viable solution in quantum control problems where gradient computation is infeasible or computationally demanding.
Abstract The Path integral Quantum Control (PiQC) algorithm was recently introduced as a new approach for computing optimal controls in continuous-time open and closed quantum systems. In this work, we adapt the PiQC algorithm to optimize parametrized quantum circuits and refer to this version of PiQC as the Gate-Based PiQC (GB-PiQC) algorithm. We apply GB-PiQC and the original continuous-time version of PiQC for ground state preparation of electronic structure problems, and benchmark them against the Variational Quantum Eigensolver, optimized using the standard Simultaneous Perturbation Stochastic Approximation (SPSA) optimizer, on a set of standard benchmark molecular Hamiltonians. For a fair comparison, we optimize the hyperparameters of the algorithms for each molecule. We find that both PiQC algorithms exhibit greater robustness than SPSA to variations in the target Hamiltonian induced by changes in interatomic distance, when hyperparameters for both methods are fixed at values tuned near equilibrium. Furthermore, PiQC algorithms also achieve superior performance compared to SPSA in most instances under this fixed-hyperparameter setting, particularly at stretched interatomic distances, where the Hartree–Fock solution becomes less accurate and its error grows relative to equilibrium.
We propose a new optimal control protocol for quantum state preparation in the presence of environmental noises based on the Most Likely Path (MLP) approach. The standard method for dealing with unknown noises in open quantum systems is via Lindblad master equation, which describes the Mean Path (MP) of noisy quantum trajectories. However, the mean path does not always faithfully represent the ensemble of trajectories, especially when the trajectory distribution is multimodal. The most likely path of quantum trajectories is extracted from stochastic path integral formulation, constructed from the joint probability of quantum statetrajectories and the noises. We study a quantum control problem of a single-qubit state preparation, controlling the qubit from an arbitrary initial state to the desired target state in the presence of a dephasing noise, where the control is the Rabi oscillation. This approach yields the analytical solution for the optimal control protocol for the Rabi drive, which is not possible using the standard MP approach. We also investigate the benefits of optimal Rabi drive by looking at the distribution of final states in the Bloch sphere; we find that the distribution of final state is concentrated around the desired target state and does not spread out over the qubit.
This paper considers some control problems for closed and open two-level quantum systems. The closed system's dynamics is governed by the Schrödinger equation with coherent control. The open system dynamics is governed by the Gorini-Kossakowski-Sudarshan-Lindblad master equation whose Hamiltonian depends on coherent control and superoperator of dissipation depends on incoherent control. For the closed system, we consider the problem of generation of the phase shift gate for some values of phases and final times for which we numerically show that zero coherent control, which is a stationary point of the objective functional, is not optimal; it gives an example of subtle point for practical solving quantum control problems. The two-stage method, which was developed in [48] for generic NNN-level open quantum systems for approximate generation of a given target density matrix, is modified here for the case of two-level systems. We modify the first ("incoherent") stage by numerically optimizing piecewise constant incoherent control instead of using constant incoherent control analytically computed using eigenvalues of the target density matrix. Exact analytical formulas are derived for the system state evolution, the objective functions and their gradients for the modified first stage. These formulas are then applied in the two-step gradient projection method. The numerical simulations show that the modified first stage duration can be significantly less than the unmodified first stage duration, but at the cost of performing optimization in the class of piecewise constant controls.
Path integral control is a stochastic optimal control framework that computes optimal policies as weighted averages over state trajectories. It was recently shown that, combined with stochastic quantum trajectories, the path integral control approach constitutes a promising alternative for quantum optimal control. In this work, we propose an extension of path integral control to the complex plane using circular complex Wiener processes. The change of measure is defined on the driving noise space under an exact control-noise matching condition, which also accommodates rank-deficient state diffusions. Applied to stochastic Schrödinger equations, the resulting formalism gives a compact treatment of paired non-Hermitian jump channels with unequal positive dissipation rates and yields cross-entropy-optimal feedback and open-loop control formulas.
This article considers some control problems for closed and open two-level quantum systems. The closed system's dynamics is governed by the Schrödinger equation with coherent control. The open system's dynamics is governed by the Gorini-Kossakowski-Sudarshan-Lindblad master equation whose Hamiltonian depends on coherent control and superoperator of dissipation depends on incoherent control. For the closed system, we consider the problem for generation of the phase shift gate for some values of phases and final times for which we numerically show that zero coherent control, which is a stationary point of the objective functional, is not optimal; it gives an example of subtle point for practical solving quantum control problems. The two-stage method, which was developed in [A. Pechen, Phys. Rev. A., 84, 042106 (2011)] for generic NNN-level open quantum systems for approximate generation of a given target density matrix, is modified here for the case of two-level systems. We modify the first ("incoherent") stage by numerically optimizing piecewise constant incoherent control instead of using constant incoherent control analytically computed using eigenvalues of the target density matrix. Exact analytical formulas are derived for the system's state evolution, the objective functions and their gradients for the modified first stage. These formulas are then applied in the two-step gradient projection method. The numerical simulations show that the modified first stage's duration can be significantly less than the unmodified first stage's duration, but at the cost of performing optimization in the class of piecewise constant controls. Bibliography: 72 titles.
This thesis investigates two central challenges for quantum computing: identifying when quantum annealing can offer a computational advantage, and developing effective methods to control realistic quantum systems. It establishes complexity bounds for an adiabatic algorithm for combinatorial optimization, showing a universal quadratic advantage while highlighting the practical difficulty of realizing the required schedule. It also introduces Path Integral Quantum Control, a trajectory-based framework for optimizing controls in open quantum systems, and develops a stochastic Hamiltonian description of continuous quantum measurement connected to double-bracket gradient flows. Together, these results advance the theoretical foundations of quantum optimization, open-system control, and measurement-based feedback