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PreprintCC BY 4.0arXiv

Error Bounds for Boundary-Stopped Positive Cubature Schemes for Hamilton--Jacobi--Bellman Equations

Abstract

We derive error bounds for a boundary-stopped positive cubature scheme for degenerate parabolic Hamilton--Jacobi--Bellman equations with Dirichlet data on bounded domains. The scheme balances antipodal branches at their first boundary contacts and uses a control-dependent effective time. Its stopped-barrier remainder is O(τΔtγ/2), and the total mass of interpolated branches is at most 2τ/Δt, where τ is the effective time. After division by the effective time, these estimates give a consistency bound that is uniform as τ→0. Under a common strict boundary barrier and the stated mesh conditions, interior consistency, coefficient shaking, switching, and localized comparison yield |(u−uh)+|∞≤ C(Δt1/4+hΔt−1/2), |(uh−u)+|∞≤ C(Δt1/10+h1/2Δt−1/4). Thus Δtasymp h10/7 gives an O(h1/7) maximum-norm bound. The analysis applies to any fixed centrally symmetric positive degree-two cubature and permits rank-deficient diffusion. Numerical examples examine parallel heat loss to a cold wall and control-dependent, rank-deficient diffusion.

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BibTeX
@misc{xu2026error,
  title = {{Error Bounds for Boundary-Stopped Positive Cubature Schemes for Hamilton--Jacobi--Bellman Equations}},
  author = {Haoran Xu and Xingye Yue},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.17186},
  eprint = {2609.17186},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.17186},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Error Bounds for Boundary-Stopped Positive Cubature Schemes for Hamilton--Jacobi--Bellman Equations
AU  - Haoran Xu
AU  - Xingye Yue
PY  - 2026
DA  - 2026/09/15
PB  - arXiv
DO  - 10.48550/arxiv.2609.17186
UR  - https://arxiv.org/abs/2609.17186
AB  - We derive error bounds for a boundary-stopped positive cubature scheme for degenerate parabolic Hamilton--Jacobi--Bellman equations with Dirichlet data on bounded domains. The scheme balances antipodal branches at their first boundary contacts and uses a control-dependent effective time. Its stopped-barrier remainder is O(τΔt^γ/2), and the total mass of interpolated branches is at most 2τ/Δt, where τ is the effective time. After division by the effective time, these estimates give a consistency bound that is uniform as τ→0. Under a common strict boundary barrier and the stated mesh conditions, interior consistency, coefficient shaking, switching, and localized comparison yield |(u−u_h)^+|_∞≤ C(Δt^1/4+hΔt^−1/2), |(u_h−u)^+|_∞≤ C(Δt^1/10+h^1/2Δt^−1/4). Thus Δtasymp h^10/7 gives an O(h^1/7) maximum-norm bound. The analysis applies to any fixed centrally symmetric positive degree-two cubature and permits rank-deficient diffusion. Numerical examples examine parallel heat loss to a cold wall and control-dependent, rank-deficient diffusion.
ER  -