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Physics-Informed Policy Iteration (PINN-PI)

Updated 3 January 2026
  • Physics-Informed Policy Iteration (PINN-PI) is a mesh-free framework that integrates physics-informed neural networks with dynamic programming to solve nonlinear optimal and stochastic control PDEs.
  • It alternates between neural network-based policy evaluation and improvement using automatic differentiation and KL-divergence loss, ensuring convergence with rigorous L2 error bounds.
  • PINN-PI demonstrates scalability and efficiency for high-dimensional systems, extending to robust control, stochastic differential games, and PDE-constrained applications.

Physics-Informed Policy Iteration (PINN-PI) is a mesh-free algorithmic framework that leverages physics-informed neural networks (PINNs) to solve nonlinear optimal control, stochastic control, and differential game problems posed as partial differential equations (PDEs) of Hamilton–Jacobi–Bellman (HJB) or Hamilton–Jacobi–Isaacs (HJI) type. PINN-PI systematically alternates between neural network-based policy evaluation and improvement, integrating automatic differentiation with classical dynamic programming constructs. The approach provides rigorous L2L^2 error bounds, ensures convergence, and demonstrates scalability for high-dimensional problems that are intractable for grid-based solvers.

1. Mathematical Formulation and Policy Iteration Paradigm

PINN-PI is grounded in the controlled diffusion framework and entropy-regularized control. For dd-dimensional stochastic systems governed by

dXt=[Ub(Xt,u)π(Xt,du)]dt+σ(Xt)dWtdX_t = \left[\int_U b(X_t,u)\,\pi(X_t,du)\right] dt + \sigma(X_t) dW_t

the entropy-regularized cost for a relaxed policy π\pi is

Vπ(x)=E[0eρt(Ur(Xt,u)π(Xt,du)λKL(π(Xt,)ρ0))dt]V^\pi(x) = \mathbb{E}\left[\int_0^\infty e^{-\rho t} \left(\int_U r(X_t,u)\,\pi(X_t,du) - \lambda\,\mathrm{KL}\left(\pi(X_t,\cdot)\Vert\rho_0\right)\right) dt\right]

where ρ0\rho_0 is a reference measure, and λ\lambda controls the regularization strength (Kim et al., 3 Aug 2025). The optimal value V(x)=supπVπ(x)V(x)=\sup_\pi V^\pi(x) solves the nonlinear elliptic entropy-regularized HJB,

$\rho V(x) = \sup_{\pi\in\Pcal(U)} \left\{\tfrac{1}{2}\mathrm{tr}\left(\Sigma(x) D^2 V(x)\right) + \int_U [b(x,u)\cdot\nabla V(x)+r(x,u)]\pi(du) - \lambda\int_U \ln\pi(u)\,\pi(du)\right\}$

Classical policy iteration alternates:

  • Policy evaluation: Solve the linear PDE for VπV^\pi given fixed π\pi.
  • Policy improvement: Derive the updated policy by softmax or minimization based on value gradients.

For general stochastic control or differential games, PINN-PI applies to HJB/HJI equations of the form

tV+H(x,V,D2V)=0\partial_t V + H(x, \nabla V, D^2 V) = 0

with Hamiltonian HH encoding supremum/infinum (or minimax) operators over controls/disturbances (Yang et al., 21 Jul 2025, Wang et al., 26 Aug 2025). In robust control, Zubov-type PDEs are handled using similar max Hamiltonian formulations.

2. PINN-Based Policy Evaluation and Neural Architecture

PINN-PI approximates both the value function V(x)V(x) and the policy π(x,u)\pi(x,u) (when needed) with neural networks. Key implementation aspects:

  • Value networks v(x;θ)v(x;\theta) and policy networks π(x,u;ω)\pi(x,u;\omega) parameterized by θ\theta, ω\omega.
  • Policy evaluation: Minimize the mean-squared PDE residual,

Lres(θ)=1Ni=1NR(xi;θ,ωn)2\mathcal{L}_{\text{res}}(\theta) = \frac{1}{N}\sum_{i=1}^N |\mathcal{R}(x_i; \theta, \omega_n)|^2

with R(xi;)\mathcal{R}(x_i; \cdot) encoding the local HJB/HJI residual (Kim et al., 3 Aug 2025, Meng et al., 2024).

  • Policy improvement: Fit the network π(x,u;ω)\pi(x,u;\omega) to the analytic target (softmax or argmin) using KL-divergence loss or supervised anchor points (Kim et al., 3 Aug 2025, Wang et al., 26 Aug 2025).
  • Collocation points {xi}\{x_i\} sampled iid in state and {uj}\{u_j\} in action space, supporting mesh-free approximation. Networks typically have 4-6 layers, 50-128 units per layer, with tanh\tanh or ReLU\text{ReLU} activations (Kim et al., 3 Aug 2025, Mukherjee et al., 2023).

3. Mesh-Free Implementation and Training Procedures

  • Mesh-free spatial sampling: N=103N=10^3 to 2×1042\times 10^4 collocation points per iteration, batch size 10310^3.
  • Automatic differentiation computes gradients and Hessians required for PDE residuals.
  • Optimization uses Adam with learning rates 10410^{-4}10310^{-3}.
  • Alternation: Each PI cycle iteratively refines θ\theta and ω\omega until the L2L^2 norm of value update v(;θn+1)v(;θn)L2\|v(\cdot; \theta_{n+1}) - v(\cdot; \theta_n)\|_{L^2} falls below tolerance (Kim et al., 3 Aug 2025, Kim et al., 3 Aug 2025).

For high-dimensional systems, direct mesh-based solvers exhibit exponential growth in complexity; PINN-PI maintains tractability across dimensions up to d=10d=10 (Meng et al., 2024, Yang et al., 21 Jul 2025).

4. Error Decomposition and Theoretical Guarantees

PINN-PI admits rigorous error bounds via a three-term decomposition:

v~nVL2(X)v~nv^nPDE residual error+v^nvnpolicy network error+vnViteration error\|\tilde v^n - V\|_{L^2(\mathcal{X})} \leq \underbrace{\|\tilde v^n - \hat v^n\|}_{\text{PDE residual error}} + \underbrace{\|\hat v^n - v^n\|}_{\text{policy network error}} + \underbrace{\|v^n - V\|}_{\text{iteration error}}

Assuming uniform ellipticity, drift bounds, and Lipschitz continuity of the policy update, the total error remains O(r+q)O(r+q) (policy network error plus PINN residual) with exponential convergence in the PI index [(Kim et al., 3 Aug 2025), Thm. 4.1; (Kim et al., 3 Aug 2025); (Yang et al., 21 Jul 2025), Thm. 3.3]. Lipschitz bounds ensure that errors in value gradients propagate linearly to policy updates.

Variants such as ELM-PI apply linear least-squares when the system dimension is small, while PINN-PI (deep networks) generalizes to high-dimensional scenarios (Meng et al., 2024).

5. Extensions to Robust Control and Differential Games

PINN-PI extends to:

  • Robust region of attraction (RROA), generalized Zubov PDE: Policy iteration alternates linear PDE solve under fixed disturbance and pointwise maximization to find optimal disturbance. Rollout-based anchor points stabilize training to prevent singular flat solutions (Wang et al., 26 Aug 2025).
  • Stochastic differential games: Policy iteration solves HJI equations via minimax optimization at the policy improvement step. The value function is approximated mesh-free, and controls/disturbances are updated via pointwise saddle-point problems leveraging automatic differentiation (Yang et al., 21 Jul 2025). Equi-Lipschitz properties ensure convergence without convexity.

6. Numerical Benchmarks and Empirical Performance

PINN-PI has demonstrated empirical scalability, accuracy, and robustness:

  • High-dimensional LQR (d=5,10d=5,10): PINN-PI achieves smooth convergence to near-optimal values, maintaining L2L^2 errors below 10210^{-2}. SAC (Soft Actor-Critic) requires orders of magnitude more data and plateaus for d=10d=10 (Kim et al., 3 Aug 2025, Kim et al., 3 Aug 2025).
  • Nonlinear benchmarks (pendulum, cartpole): PINN-PI stabilizes in fewer iterations, handles strong noise, and achieves higher rewards than model-free RL algorithms (Kim et al., 3 Aug 2025, Kim et al., 3 Aug 2025).
  • Fluid-cooled battery packs (1D coupled PDE): Hybrid PINN-PI actor-critic framework attains fourfold improvement in sample efficiency compared to PPO, exploiting physical structure in the value network (Mukherjee et al., 2023).
  • Robust region of attraction (2D Van der Pol, 10D decoupled): Rollout-enhanced PINN-PI achieves contour-accurate RROA estimates, avoiding singularities and scaling to d=10d=10 (Wang et al., 26 Aug 2025).
  • Differential games (publisher-subscriber, path planning): PINN-PI outperforms direct PINN solvers in accuracy and smoothness, maintaining relative L2L^2 errors <102<10^{-2} in d=5,10d=5,10 (Yang et al., 21 Jul 2025).

Sample performance metrics:

Benchmark Dimensionality PINN-PI L2L^2 error Reference method Data efficiency
LQR $5,10$ <102<10^{-2} SAC \gg lower
Cartpole $2$ Higher reward SAC Faster converg.
Zubov (decoupled) $10$ Accurate contours FDM Matched
Publisher-Subscr. $5,10$ 102,5×10210^{-2}, 5\times10^{-2} Direct PINN Superior

PINN-PI maintains polynomial runtime scaling in practice, with wall-clock times comparable or superior to SAC and dramatically better than grid-based solvers as dd increases (Kim et al., 3 Aug 2025, Meng et al., 2024).

7. Rigorous Verification, Stability, and Application Domains

Stability certification via formal verification (SMT solvers such as dReal) permits Lyapunov-region guarantees for the learned controllers, especially in nonlinear settings (Meng et al., 2024).

PINN-PI is applicable across domains:

A plausible implication is that direct embedding of physical PDE structure and dynamic programming into neural policy iteration yields scalable, verifiable control solutions robust to dimensionality and model regularization requirements.

References

  • "Physics-informed approach for exploratory Hamilton--Jacobi--Bellman equations via policy iterations" (Kim et al., 3 Aug 2025)
  • "Neural Policy Iteration for Stochastic Optimal Control: A Physics-Informed Approach" (Kim et al., 3 Aug 2025)
  • "Solving nonconvex Hamilton--Jacobi--Isaacs equations with PINN-based policy iteration" (Yang et al., 21 Jul 2025)
  • "Learning Robust Regions of Attraction Using Rollout-Enhanced Physics-Informed Neural Networks with Policy Iteration" (Wang et al., 26 Aug 2025)
  • "Physics-Informed Neural Network Policy Iteration: Algorithms, Convergence, and Verification" (Meng et al., 2024)
  • "Actor-Critic Methods using Physics-Informed Neural Networks: Control of a 1D PDE Model for Fluid-Cooled Battery Packs" (Mukherjee et al., 2023)

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