A Structural Pseudo-Hermitian Toy Model of Spontaneous Symmetry Breaking in Non-Orientable Phase Domains

This preprint presents a pseudo-Hermitian lattice toy model based onnon-orientable topological structures, with results organised accordingto a strict epistemological hierarchy separating proved results, controlled approximations, structural analogies, and speculativeextensions. The work should be interpreted as a structured mathematical thoughtexperiment rather than a complete physical theory. Its primary objectiveis to establish a minimal, exactly solvable framework in whichnon-orientable topology, pseudo-Hermitian dynamics, spectral doubling, and topological classification coexist in a single 2×2 matrix model. ─────────────────────────────────────────────DIMENSIONAL STRUCTURE───────────────────────────────────────────── The rigorous model (Levels 1–2) is defined on a one-dimensional spatiallattice with a two-component internal space ℂ². No temporal variableexists at this level. The identification of the internal degree offreedom with a temporal direction is a Level 3–4 conjecture, explicitlyseparated in the paper. The continuum field equation containing ∂ₜ isan embedding ansatz, not a derived result; the spectral convergenceresults concern the spatial Hamiltonian only. ─────────────────────────────────────────────VERIFIED RESULTS (Level 1, proved to machine precision ~10⁻¹⁵) ───────────────────────────────────────────── • The Möbius lattice carries a global Pin⁺ structure, proved via ℤ₂ CW-complex homology and obstruction theory. In one spatial dimension, H² (ℳN; ℤ₂) = 0 and the obstruction vanishes automatically; the antilinear operator 𝒯² = +𝕀 selects Pin⁺ over Pin⁻. • The model belongs to Altland–Zirnbauer symmetry class BDI† (not standard BDI), with a ℤ winding number invariant in one spatial dimension. The chiral operator satisfies S² = −𝕀 and S ≠ 𝒯𝒞, a genuine non-Hermitian feature absent in the Hermitian classification. • The absence of the σ₂ Pauli component in the effective Hamiltonian is a structural consequence of the chiral symmetry forced by the Möbius boundary conditions, not a basis choice. • The exceptional-point surface is a stratified topological inversion boundary: all BDI† symmetries persist at machine precision in all three regions (exterior, exceptional point, interior). The topological structure is operationally inaccessible but not annihilated in the broken phase — a result with no direct Hermitian analogue. • The GBZ (Generalized Brillouin Zone) winding number WGBZ = −1 has been verified numerically via the deformed contour det H (k+iε), with convergence to integer precision for all ε > 0 tested. The model is in the topological phase for the reference parameters (t=1, m=2, λ=0. 5). The open problem is the biorthogonal formulation in the broken phase, where the biorthogonal basis collapses and WGBZ is not derivable from the spectral decomposition. • Convergence of the effective mass to its continuum value scales as 𝒪 (1/N), and the effective velocity scales as 𝒪 (1/N²), verified on N = 4, 8, 16, 32, 64. ─────────────────────────────────────────────CONTROLLED RESULTS (Level 2) ───────────────────────────────────────────── • Dirac-like effective Hamiltonian derived from the lattice with explicit error bounds. • Nambu re-embedding structurally consistent with the pseudo-Hermitian framework. The ∂ₜ in the continuum embedding is introduced by the standard substitution E → iℏ∂ₜ; its extension to a full (1+1) D field equation is the Level 3 step. ─────────────────────────────────────────────STRUCTURAL ANALOGIES (Level 3) ───────────────────────────────────────────── • Higgs-like spectral reduction formalised as an operator-algebra isomorphism. • Majorana-like structure correctly classified as class BDI†, distinct from Kitaev class D. • The pixel/antipixel doubling of the internal space ℂ², enforced by the Möbius boundary conditions, produces a structural analogue of time-reversal doubling. The identification of the two sectors with forward/backward temporal orientations is an algebraic isomorphism, not a physical derivation. ─────────────────────────────────────────────SPECULATIVE EXTENSIONS (Level 4, clearly separated) ───────────────────────────────────────────── • Wheeler–DeWitt cosmological limit interpreted as a global exceptional point where E₊ = E₋ = 0. • Gravitational geometrogenesis and emergent time (chronostereogenesis) as long-range conjectures. • Extension to a (1+3) D geometry via a compact non-orientable 4-manifold (e. g. ℝP⁴ or 𝒦×𝒦), where the Pin⁺/Pin⁻ distinction is equivalent to the CPT structure of the physical theory (Atiyah 1971). ─────────────────────────────────────────────REFERENCE MODEL MAPPINGS───────────────────────────────────────────── The model is mapped explicitly onto three reference systems: • PT-symmetric quantum chains — exact isomorphism• Non-Hermitian SSH model — partial correspondence (at k=0, π only) • Kitaev BdG chain — non-isomorphic; distinct AZ class (D vs BDI†) ; the imaginary coupling iλ vs real Δ changes 𝒞² from −1 to +1 and no unitary transformation bridges the two ─────────────────────────────────────────────WHAT THE FRAMEWORK DOES NOT YET PROVIDE───────────────────────────────────────────── • A rigorous continuum-limit derivation beyond the controlled 𝒪 (1/N) approximation. • A complete gauge-invariant quantum field formulation. • A full recovery of Lorentz symmetry. • A dynamically fluctuating geometric sector. • Experimentally testable phenomenology beyond synthetic platform predictions. ─────────────────────────────────────────────PRIMARY OPEN PROBLEMS AND INVITATION TO COLLABORATE───────────────────────────────────────────── The exactly solvable 1D model is the rigorous baseline for the followinghierarchy of generalisations on non-orientable manifolds: ℳ (Möbius) → 𝒦 (Klein bottle) → ℝP³ → X⁽⁴⁾ (I) Pin obstruction on the Klein bottle (2D) — entry level, algebraic topology. In 1D the obstruction H² (ℳN; ℤ₂) = 0 is automatic. On 𝒦, H² (𝒦; ℤ₂) ≅ ℤ₂ ≠ 0 and the obstruction w₂ ± w₁² may be non-trivial. Does a global Pin structure exist, and of which type? (II) AZ classification in 2D non-orientable geometry — intermediate. Standard Bott periodicity predicts a trivial (0) invariant for class BDI in 2D. Does non-orientable topology restore a non-trivial (ℤ or ℤ₂) invariant? Does the model remain in class BDI†? (III) Biorthogonal winding number in the broken phase — intermediate. WGBZ = −1 is verified via GBZ deformation. The open problem is the fully biorthogonal formulation (cf. Shen et al. 2018; Kunst–Dwivedi 2019) where the biorthogonal basis has collapsed, possibly via a transfer-matrix approach. (IV) Pseudo-Hermitian Hamiltonian on a compact non-orientable 4-manifold and the CPT connection — advanced. In 4D, Pin⁺ vs Pin⁻ is equivalent to the CPT structure (Atiyah 1971). Class BDI in 4 spatial dimensions carries a ℤ invariant. This is the primary open problem for the chronostereogenesis programme in (1+3) D. (V) Experimental observation of the stratified exceptional-point cascade in photonic lattices — experimental. The parameters (t, m, λ) map directly onto coupled waveguide arrays. For N=4: two-step cascade at λc ≈ 0. 59 and 3. 41 (for t=1, m=2). Can the hierarchical mode coalescence be resolved experimentally? (VI) Second quantisation and dynamic coupling — advanced. Construction of the multi-particle operator field theory and U (1) gauge embedding within the non-orientable topology. Each problem has an independent entry point. Collaboration is welcomedfrom researchers in algebraic topology, non-Hermitian condensed mattertheory, mathematical physics (spin geometry), experimental photonics, and quantum gravity / geometrogenesis. ─────────────────────────────────────────────INTENDED SCOPE───────────────────────────────────────────── This work is intended as an open exploratory framework. Its publicationaims to stimulate mathematical discussion, critical analysis, andpotential interdisciplinary collaboration in mathematical physics, topological quantum systems, non-Hermitian mechanics, and emergentgeometry. The 1D model presented here was designed to be exactlysolvable precisely so that its extensions would be well-posed: therigorous kernel provides the baseline against which anyhigher-dimensional generalisation can be tested.