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PreprintCC BY-SA 4.0arXiv

Stability in the determination of the coefficients for coupled relativistic Schrödinger system

Abstract

In this article, we prove a stability result for the identification of the coefficients appearing in a coupled relativistic Schrödinger system posed on a bounded domain of ℝ1+n, where n ≥ 3. More precisely, by utilizing input-output operator, where Neumann boundary data are available only on a subset of the boundary, and constructing an appropriate geometric optics solution, we derive a stability estimate of log-log type for the matrix-valued first-order coefficients. This result is subsequently used to obtain a log-log-log type stability estimate for the zeroth-order matrix-valued potential.

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BibTeX
@misc{kumar2026stability,
  title = {{Stability in the determination of the coefficients for coupled relativistic Schrödinger system}},
  author = {Nitesh Kumar and Parveen Kumar and Tanmay Sarkar},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.15013},
  eprint = {2610.15013},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.15013},
  note = {CC BY-SA 4.0},
}
RIS
TY  - UNPB
TI  - Stability in the determination of the coefficients for coupled relativistic Schrödinger system
AU  - Nitesh Kumar
AU  - Parveen Kumar
AU  - Tanmay Sarkar
PY  - 2026
DA  - 2026/10/10
PB  - arXiv
DO  - 10.48550/arxiv.2610.15013
UR  - https://arxiv.org/abs/2610.15013
AB  - In this article, we prove a stability result for the identification of the coefficients appearing in a coupled relativistic Schrödinger system posed on a bounded domain of ℝ^1+n, where n ≥ 3. More precisely, by utilizing input-output operator, where Neumann boundary data are available only on a subset of the boundary, and constructing an appropriate geometric optics solution, we derive a stability estimate of log-log type for the matrix-valued first-order coefficients. This result is subsequently used to obtain a log-log-log type stability estimate for the zeroth-order matrix-valued potential.
ER  -