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Schur elimination of brane-localised Higgs mass spectra, and the criteria for the $ε\to0$/$N\to\infty$ non-commutativity
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 di
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