The theorem excited_jcost in module IndisputableMonolith.Physics.RecognitionHamiltonianSpectrum states:
theorem excited_jcost {r : ℝ} (hr : 0 < r) (hne : r ≠ 1) :
0 < Jcost r := Jcost_pos_of_ne_one r hr hne
This asserts that the recognition cost function Jcost is strictly positive for every positive real ratio r distinct from unity. In the Recognition Hamiltonian Spectrum, the vacuum sector is defined by Jcost 1 = 0 (see vacuum_jcost). The excited_jcost theorem therefore separates all excited sectors (J > 0) from the ground state. The module packages this into HamiltonianSpectrumCert, whose excited field is exactly the universal quantification given by excited_jcost. The same positivity is reused to witness a positive spectral gap on any discretized lattice with spacing a > 0 (see lattice_gap_witness). The five-sector decomposition (vacuum, goldstone, massiveScalar, massiveVector, massiveTensor) follows independently from spectralSectorCount.