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The Higgs condensates are proven along with the minimal versions of the hyper-symmetric 2HDM extensions when containing Supersymmetry that can play the role of oscillators for the CPC and CPV interferences, up to via τ 2 . With the uncharged Higgs inclusion (considering the uncharged Goldstone Bosons compared to the spontaneously broken SM-like Higgs), the symmetric H T and anti-symmetric H S linear combinations of an ' H u ' and a rescaled H d ′ = (3 2) 2 3 H d , where masses of m H d ′ ≅ m H SM ≈ 1 2 5 GeV and m H d = (2 3) 2 3 m H u ≈ 9 5 GeV, such as under the condensate's boundary impacts. The range of the H d ′ s would be up to where the composed singlet and triplet can interchange, then, they approach the Custodial SUSY at a Triple point transition with a Goldstone-type order mass m S 0 ≈ 0. 3 4 GeV, as well into their Dark Matter sectors' cut-off Λ , (including m T ) up to order 1.7 TeV. That will lead to opening the way to measure the existence of Supersymmetry, indirectly at the least, through any dominance of Z 2 -violating Higgs decays. [ABSTRACT FROM AUTHOR]

A limiting algebraic resonance seems to recuperate the pseudo-scalar Higgs from the simultaneous breaking process. On an energy kernel consideration, an imposed nonharmonic boundary exclusion provides a basis for the scaling (proved derived from the conformal classes) of its extending as radiative correction diagrams, plus whose anomalies eliminate upon reaching geometrically a type of steep power as linked to, completely from the curvature. A CP violating form, then shows after the appearance of both a parity, plus a polarization defiance, together with the Higgs decoupled to the favor of the equivalence class for a scalar coupling, leading to the types of allowed UV fixed points, with the possible fading of some of its parametric resonances (tachyon) by quantum corrections, into then the estimation of consecutive QCD and fuzzy axion masses by taking into account that their interaction (dimensional) operators such which have the completeness, both of metric and/or gauge types, being so then, first with KSVZ (showing as being resonant along with sterile neutrinos) and DFS types or second with creation of an axion soliton. The fit into the phenomenological constraints is also checked. [ABSTRACT FROM AUTHOR]