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A method of moving planes for a mixed local-nonlocal parabolic system with quenching

Abstract

In this paper we develop a parabolic version of the method of moving planes on systems with a mixed local and nonlocal diffusion operator, that being ℒ = −(−Δ)s + Δ, where (−Δ)s is the integral fractional laplacian. We then use this result to study the quenching phenomena occurring in said systems with a singular absorption term of the type (1−u)−p. We prove that there exists a range of multiplicative parameters for which every solution presents quenching, and that for any initial datum u0, there exists a small enough multiplicative parameter such as the solution is globally defined. We also prove that the quenching phenomena cannot happen arbitrarily close to the boundary, but they are contained in a compact subset of the domain.

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BibTeX
@misc{junquera2026method,
  title = {{A method of moving planes for a mixed local-nonlocal parabolic system with quenching}},
  author = {Sergio Junquera and Leandro M. Del Pezzo},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.08014},
  eprint = {2610.08014},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.08014},
}
RIS
TY  - UNPB
TI  - A method of moving planes for a mixed local-nonlocal parabolic system with quenching
AU  - Sergio Junquera
AU  - Leandro M. Del Pezzo
PY  - 2026
DA  - 2026/10/06
PB  - arXiv
DO  - 10.48550/arxiv.2610.08014
UR  - https://arxiv.org/abs/2610.08014
AB  - In this paper we develop a parabolic version of the method of moving planes on systems with a mixed local and nonlocal diffusion operator, that being ℒ = −(−Δ)^s + Δ, where (−Δ)^s is the integral fractional laplacian. We then use this result to study the quenching phenomena occurring in said systems with a singular absorption term of the type (1−u)^−p. We prove that there exists a range of multiplicative parameters for which every solution presents quenching, and that for any initial datum u_0, there exists a small enough multiplicative parameter such as the solution is globally defined. We also prove that the quenching phenomena cannot happen arbitrarily close to the boundary, but they are contained in a compact subset of the domain.
ER  -