Schur elimination of brane-localised Higgs mass spectra, and the criteria for the ε→0/N→∞ non-commutativity

@misc{barcelo2026schur,
  title = {{Schur elimination of brane-localised Higgs mass spectra, and the criteria for the $ε\to0$/$N\to\infty$ non-commutativity}},
  author = {Roberto Barceló and Subhadip Mitra},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.39910},
  eprint = {2609.39910},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.39910},
}

TY  - UNPB
TI  - Schur elimination of brane-localised Higgs mass spectra, and the criteria for the ε→0/N→∞ non-commutativity
AU  - Roberto Barceló
AU  - Subhadip Mitra
PY  - 2026
DA  - 2026/09/30
PB  - arXiv
DO  - 10.48550/arxiv.2609.39910
UR  - https://arxiv.org/abs/2609.39910
AB  - In many 5D extensions of the Standard Model, the Higgs boson is localised to a single point along the extra dimension, where it couples to bulk fermions. Computing the fermion mass spectrum then requires a boundary regulator, and removing it before or after summing the Kaluza-Klein tower can give different answers, as shown in Ref.~\cite{Barcelo:2014kha}. Because the coupling reaches any KK mode through only two overlap numbers, the whole tower can be eliminated exactly by a Schur complement; the disagreement between the two orders of limit then reduces to a single sum, whose discontinuity we prove directly. This discontinuity needs two conditions to appear: a coupling sharp enough to leave the sum conditionally convergent, and a second channel with complementary behaviour at the point of contact. Neither condition depends on having an extra dimension, or even a discrete tower to sum. The same test applies to contact interactions in ordinary scattering, the imaginary part behind the optical theorem, and seesaw, portal, and clockwork constructions. Whether the two conditions are met determines whether a similar ambiguity plays any role.
ER  -