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Nonsmooth Obstacles and Killed Resolvents in Reflected Stochastic Control

Published 19 Jun 2026 in math.OC and math.PR | (2606.21575v1)

Abstract: We study an infinite-horizon optimal stopping problem for a normally reflected two-dimensional diffusion in the quadrant with nonsmooth max-type payoff (G(x_1,x_2)=x_1\veeαx_2). The main novelty is a measure-valued variational formulation: the stopping gain (Γ=c+rG-\mathcal LG) is shown to be a signed Radon measure whose singular component is supported on the kink diagonal ({x_1=αx_2}), and this component is computed explicitly. We prove that the value admits the killed-resolvent representation [ V=G-R_r{\mathcal C}Γ, ] where the reflected diffusion is killed upon entry into the stopping set. This corrects the generally invalid unrestricted-resolvent formula. Under explicit monotonicity hypotheses, the stopping set has epigraph form, and the free boundary is characterized by a killed-potential trace condition. A verification theorem certifies locally Lipschitz candidate boundaries as optimal.

Authors (3)

Summary

  • The paper establishes that nonsmooth max-type payoffs in reflected stochastic control require a measure-valued obstacle approach to properly capture singularities.
  • The authors leverage a killed-resolvent representation to ensure correct free-boundary determination, validated by numerical simulations and Monte Carlo experiments.
  • The study demonstrates parameter sensitivity effects, showing that excluding the diagonal singular measure introduces significant boundary errors.

Measure-Valued Variational Formulation in Reflected Stochastic Optimal Stopping

Problem Context and Formulation

The paper "Nonsmooth Obstacles and Killed Resolvents in Reflected Stochastic Control" (2606.21575) presents a rigorous analysis of an infinite-horizon optimal stopping problem driven by a two-dimensional, normally reflected diffusion in the positive quadrant R+2\mathbb{R}_+^2. The objective is to maximize expected discounted rewards given by a nonsmooth, convex max-type payoff G(x1,x2)=x1αx2G(x_1, x_2) = x_1 \vee \alpha x_2, subject to a running cost cc and discount rate rr. The dynamic is governed by the reflected SDE:

dXt=b(Xt)dt+σ(Xt)dWt+dLt,dX_t = b(X_t)\,dt + \sigma(X_t)\,dW_t + dL_t,

where LtL_t enforces normal reflection at the boundary. The primary analytic peculiarity arises from the nonsmoothness of GG, whose kink at the diagonal Δ={x1=αx2}\Delta = \{x_1 = \alpha x_2\} induces singular behavior in associated variational and potential-theoretic representations.

Measure-Valued Obstacle and Stopping Gain

The value function for the optimal stopping problem is characterized as the solution to a reflected variational inequality:

max{LVrVc,GV}=0\max\{\mathcal{L} V - r V - c, G - V\} = 0

with normal reflection on {xi=0}\{x_i = 0\} for G(x1,x2)=x1αx2G(x_1, x_2) = x_1 \vee \alpha x_20, where G(x1,x2)=x1αx2G(x_1, x_2) = x_1 \vee \alpha x_21 is the generator for the diffusion. The nonsmooth nature of G(x1,x2)=x1αx2G(x_1, x_2) = x_1 \vee \alpha x_22 prohibits standard G(x1,x2)=x1αx2G(x_1, x_2) = x_1 \vee \alpha x_23 analytic techniques; crucially, the obstacle's singularity on G(x1,x2)=x1αx2G(x_1, x_2) = x_1 \vee \alpha x_24 forces the stopping gain G(x1,x2)=x1αx2G(x_1, x_2) = x_1 \vee \alpha x_25 to be interpreted as a signed Radon measure. The singular component localized at G(x1,x2)=x1αx2G(x_1, x_2) = x_1 \vee \alpha x_26 is explicitly computed via distributional calculus, yielding:

G(x1,x2)=x1αx2G(x_1, x_2) = x_1 \vee \alpha x_27

where G(x1,x2)=x1αx2G(x_1, x_2) = x_1 \vee \alpha x_28 and G(x1,x2)=x1αx2G(x_1, x_2) = x_1 \vee \alpha x_29 denotes surface measure on cc0. This term provides the measure-valued analogue of the local time accumulated by cc1 at zero, essential for precise modeling near the kink. Figure 1

Figure 1

Figure 1: Baseline model; left, continuation region cc2 (shaded), stopping region cc3, free boundary cc4, and diagonal cc5; right, stopping advantage cc6.

Killed Resolvent Representation

A major conceptual and practical advance is the killed-resolvent representation:

cc7

where cc8 denotes the resolvent operator for the reflected diffusion, killed upon entry to the stopping set cc9. This formula corrects the usual unrestricted-resolvent identity, which erroneously includes post-stopping occupation—an error that results in both analytic inconsistency and incorrect boundary determination. The representation employs the full measure-valued stopping gain, including both absolutely continuous and singular components, and is validated via both deterministic PDE solvers and path-space Monte Carlo estimators. Figure 2

Figure 2: (a) Monte Carlo value rr0 at the free boundary against FD value rr1; (b) Diagonal local-time potential rr2 via deterministic and MC local-time estimators.

Free-Boundary Characterization and Verification

Under explicit monotonicity assumptions—vertical monotonicity of the stopping advantage and nonemptiness of vertical stopping sections—the stopping set admits an epigraph representation:

rr3

with rr4 constituting the free boundary. The boundary is characterized not via classical smooth fit but by a killed-resolvent trace condition:

rr5

The paper formalizes this as a verification theorem: if a candidate boundary rr6 yields rr7 satisfying domination, contact, strict continuation, normalized reflection, admissible growth, and measure-superharmonicity, then rr8 coincides with the true value and the corresponding stopping time is optimal. This framework provides a rigorous certification protocol for free-boundary candidates.

Numerical Implementation and Diagnostic Experiments

The theoretical formulation is substantiated with detailed numerical analysis, combining deterministic solvers for the variational inequality and MC simulations for killed resolvent potentials. The key computational findings are:

  • Effect of the diagonal singular measure: Omitting rr9 incurs substantial boundary error (dXt=b(Xt)dt+σ(Xt)dWt+dLt,dX_t = b(X_t)\,dt + \sigma(X_t)\,dW_t + dL_t,0 in baseline tests), falsifies domination (dXt=b(Xt)dt+σ(Xt)dWt+dLt,dX_t = b(X_t)\,dt + \sigma(X_t)\,dW_t + dL_t,1 is violated), and collapses the continuation region near dXt=b(Xt)dt+σ(Xt)dWt+dLt,dX_t = b(X_t)\,dt + \sigma(X_t)\,dW_t + dL_t,2. Figure 3

Figure 3

Figure 3: Effect of the diagonal singular measure; left, true boundary dXt=b(Xt)dt+σ(Xt)dWt+dLt,dX_t = b(X_t)\,dt + \sigma(X_t)\,dW_t + dL_t,3 vs dXt=b(Xt)dt+σ(Xt)dWt+dLt,dX_t = b(X_t)\,dt + \sigma(X_t)\,dW_t + dL_t,4; right, vertical sections dXt=b(Xt)dt+σ(Xt)dWt+dLt,dX_t = b(X_t)\,dt + \sigma(X_t)\,dW_t + dL_t,5 at dXt=b(Xt)dt+σ(Xt)dWt+dLt,dX_t = b(X_t)\,dt + \sigma(X_t)\,dW_t + dL_t,6.

  • Killed vs unrestricted resolvent: The unrestricted resolvent dXt=b(Xt)dt+σ(Xt)dWt+dLt,dX_t = b(X_t)\,dt + \sigma(X_t)\,dW_t + dL_t,7 fails to satisfy the contact condition, with the candidate value exceeding dXt=b(Xt)dt+σ(Xt)dWt+dLt,dX_t = b(X_t)\,dt + \sigma(X_t)\,dW_t + dL_t,8 throughout the stopping region—demonstrating the necessity of the killed operator.
  • Parameter sensitivity: The contribution of the diagonal singular measure varies with the crossing coefficient dXt=b(Xt)dt+σ(Xt)dWt+dLt,dX_t = b(X_t)\,dt + \sigma(X_t)\,dW_t + dL_t,9 (controlled via covariance structure and payoff weight LtL_t0); as LtL_t1, LtL_t2 vanishes, directly verifying the theoretical link between correlation, singularity, and boundary location. Figure 4

    Figure 4: Boundary discrepancy LtL_t3 as a function of crossing coefficient LtL_t4 (varied via correlation LtL_t5); diagonal effect vanishes as LtL_t6.

Practical and Theoretical Implications

The measure-valued obstacle formulation establishes that nonsmooth payoffs require precise treatment of singularities in reflected stochastic control. The killed-resolvent trace condition provides a robust approach for free-boundary determination and verification, avoiding pitfalls inherent in scalar, pointwise generator calculations or unrestricted resolvent approximations. Computationally, successful implementation demands explicit inclusion of pathwise local time and careful handling of singular measures.

The theoretical framework can readily support further generalizations, including oblique reflection in polyhedral domains, higher-dimensional max-type payoffs (yielding singular measures on multiple interfaces), and relaxation of monotonicity assumptions via advanced PDE techniques.

Conclusion

The paper rigorously demonstrates that reflected optimal stopping with nonsmooth max-type payoff is governed by a measure-valued obstacle problem. The interplay between reflection, nonsmooth obstacles, and singular stopping gains induces nonlocal, killed-resolvent free-boundary equations. Both analytic and computational evidence confirms that ignoring the measure-valued structure—whether via classical generator methods or unrestricted resolvent formulas—results in invalid value representations and boundaries. The verification theorem, coupled with explicit diagnostic experiments, establishes a principled pathway for optimal boundary certification in multidimensional reflected diffusion settings with nonsmooth rewards.

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