Self-Referential Scattering Networks: Connection Matrix Synthesis, J-Unitary Robustness, and Floquet Band-Edge Topology
Abstract
In Self-Referential Scattering Networks (SSN), this paper provides closed-loop methodology from design--implementation--readout--falsification to theorem-level guarantees. Under trace-class calibration, establish mod-two equivalence between global half-phase (\det covering) holonomy, spectral shift, spectral flow through -1, and discriminant transversality. Compared to previous draft, this version completes verifiable details and checkable constants at five key junctures: (i) Section 3 adds brid
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Self-Referential Scattering Networks: Connection Matrix Synthesis, J -Unitary Robustness, and Floquet Band-Edge Topology Haobo Ma 1 Wenlin Zhang 2 1 Independent Researcher 2 National University of Singapore Version 1.10 Abstract In Self-Referential Scattering Networks (SSN), this paper provides closed-loop methodology from designimplementationreadoutfalsication to theorem-level guarantees . Under trace-class calibration , establish mod-two equivalence between global half-phase ( √det covering) holonomy, spectral shift, spectral ow through −1 , and discriminant transversality. Compared to previous draft, this version completes veriable details and checkable constants at ve key junctures: (i) Section 3 adds bridging lemma for log det regularization BirmanKren −1 spectral owmod-two intersection number with half-page self-contained proof ; (ii) Section 4 provides quantitative structural lemma for no spurious crossing after star product, specifying comparison principle and design line for principal block minimal gradient gmin and mutual coupling upper bound rmax ; (iii) Section 5 formulates binarized projection + majority voting as concentration inequality , providing explicit relation between misclassication rate and sample number with correlation correction ; (iv) Section 6 characterizes robust domain via J -inner-product normalized imaginary Rayleigh quotient (Kren angle) , constructs polarization homotopy , provides feasible upper bound for threshold function ε0(η, β) , uniformly ensuring Cayley denominator invertibility and discriminant non-crossing; (v) Section 7 formulates phase-type Floquet index truncation independence and gauge independence as theorems, completing regularization consistency and failure detection via det2 in HilbertSchmidt scenario . Engineering side provides simulatable Schur-closed form for two-port couplermicroringgain prototype, quantifying square-root scaling and threshold selection basis for group delay double-peak merging. Keywords : Closed-loop scattering; Redheer star product; Schur complement; Herglotz/Nevanlinna; discriminant; spectral shift and spectral ow; mod-two Levinson; J -unitary; Kren angle; Floquet phase-type index. 1 Calibration and Basic Objects Frequency domain and variables : ω as angular frequency (static ω∈R ; periodic systems ω∈[−π/T, π/T] ), upper half-plane calibration takes z=ω+ i0+ . Exchange with unit circle calibration via Cayley map when necessary, maintaining orientation consistency. Scattering and star product : Portized node scattering Sj(z) through interconnection (including feedback) yields closed-loop S⟲(z) via Redheer star product and Schur complement. Cayley duality (unied notation): S⟲(z)=(I−iK(z))(I+ iK(z))−1, K(z) = −iI+S⟲(z)−1I−S⟲(z). 1
Trace-class and regularization : All results related to spectral shift ξ and BirmanKren uniformly assume S⟲−I∈S1 using det . For innite dimensions (e.g., Floquet sidebands) rst truncate nitely, use det2 when necessary; this paper's mod-two conclusions independent of det /det2 choice (see Appendix F). J -unitary calibration : J=J†=J−1 , S♯=J−1S†J , S†JS =J . Non-Hermitian robustness stated under this calibration. 2 Discriminant, Local Model, and Transversality On parameter manifold X dene codimension-one piecewise smooth submanifold family D=FbDb , whose local models include Jost zeros, threshold opening/closing, embedded eigenvalues, and EP coalescence. After removal X◦=X\D . For closed path γ⊂X◦ , mod-two intersection number I2(γ, D) is parity of transverse points. Endpoints/thresholds excised via small semicircles merged into D boundary component. Closed-loop implementation level can use D=n(ω, ϑ) : σminI−C(ω, ϑ)Sii(ω, ϑ)= 0o, equivalent to det(I−CSii)=0 at general position. 3 Mod-Two Half-PhaseSpectral-ShiftSpectral-FlowIntersection: Bridging Lemma and Equivalence Theorem (Trace-Class) Denition 1 (3.1: Global Half-Phase) . ν√det S⟲(γ) = expiIγ 1 2d arg det S⟲∈ {±1}. Lemma 2 (3.2: log det Regularization and Endpoint Treatment) . If along closed path γ almost everywhere S⟲ unitary with S⟲−I∈S1 , then log det S⟲ admits continuous continuation along γ and is integrable; after treating endpoints/thresholds per 2 small semicircle excision rule, Hγ 1 2d arg det S⟲ well-dened ( mod 2π ). Lemma 3 (3.3: BirmanKren −1 Spectral Flow Bridge: Two-Step Veriable Details) . Denote ξ(ω) as spectral shift. Then (i) By BK formula det S(ω) = exp{−2πiξ(ω)} , arbitrary branch change makes ξ7→ ξ+n ( n∈Z ), contributing exp{iH1 2d(2πn)}= 1 to half-phase, thus mod-two invariant ; (ii) Let S(τ) = V(τ)eiΦ(τ)U(τ) be local Schur form with at τ=τc only one simple eigenphase ϕj crossing π ( −1 ), then ξ jump is ±1 while Sf−1= 1 . Multiple crossings decompose into nite simple crossings, thus exp−iπIγ dξ= (−1)Sf−1(S⟲◦γ). Proposition 4 (3.4: Base-Point and Branch Independent Mod-Two Property) . For arbitrary base point and continuous branch continuation, ν√det S⟲(γ) invariant; allowed endpoint treatment equivalent to adding boundary homotopy on D , mod-two value preserved. Theorem 5 (3.5: Four-Fold Equivalence) . If along γ almost everywhere S⟲ unitary with S⟲−I∈ S1 , then ν√det S⟲(γ) = exp−iπIγ dξ= (−1)Sf−1S⟲◦γ= (−1)I2(γ,D). 2
4 No Spurious Crossing After Star Product and Z2 Combinatorial Law (Quantitative Version) Block notation : S(k)= S(k) ee S(k) ei S(k) ie S(k) ii !, k = 1,2. Lemma 6 (4.1: Structural Lemma for No Spurious Crossing: Quantitative Conditions with Tubular Separation) . Assume in neighborhood U⊂X◦ satisfying (i) Schur invertibility lower bound: σminI−S(1) ii S(2) ii ≥δ > 0 ; (ii) Mutual coupling smallness: ∥S(1) ei ∥2,∥S(2) ie ∥2≤ρ < 1 ; (iii) Tubular separation : For zero sets D(k) of k= 1,2 exists uniform tubular radius τ∗>0 , take 0< τ ≤τ∗ such that Nτ(D(1)) , Nτ(D(2))⊂U and disjoint. Dene principal discriminant Φk(ϑ) = detI−CS(k) ii and principal block minimal gradient gmin = inf ϑ∈Umin|∇ϑΦ1(ϑ)|,|∇ϑΦ2(ϑ)|. Then mutual coupling residual upper bound exists rmax ≤∥S(1) ei ∥2∥S(2) ie ∥2 δ2, and when rmax <(τgmin)2 network discriminant is transverse disjoint union of subnet discriminants: Dnet =D(1) ⊔D(2) , with I2(γ, Dnet) = I2(γ, D(1)) + I2(γ, D(2)) mod 2. Proof essentials : By tubular separation and mean value theorem, outside tubes have |Φ1(ϑ)| ∧ |Φ2(ϑ)| ≥ τgmin , thus |Φ1(ϑ)Φ2(ϑ)| ≥ (τgmin)2 ; when rmax <(τgmin)2 , mutual coupling remainder insucient to introduce new zeros outside tubes. In each single tube use implicit function theorem obtaining zero set as normal small deformation of original zero set, obtaining transverse disjoint union since tubes non-intersecting. Engineering design line (veriable) Take δ= infUσmin(I−S(1) ii S(2) ii ) . If ∥S(1) ei ∥2∥S(2) ie ∥2≤1 2δ2(τgmin)2, then rmax ≤1 2(τgmin)2<(τgmin)2 , satisfying lemma sucient condition. Boundary and failure mode 4.2 : When δ→0+ or ρ→1− , near-tangent crossing and resonance-induced spurious crossing may occur. Should real-time monitor σmin(I−CSii) margin and gmin numerical estimate, shrink U or recongure ports when necessary. Theorem 7 (4.3: Z2 Combinatorial Law) . Under lemma conditions, νnet =ν(1) ⊙ν(2) (componentwise multiplication, mod-two addition). 3
5 Binarized Projection, Concentration Inequality, and Dealiasing Phase increment and binarization : ∆ϕab =1 2harg det Sγa;θb+δ−arg det Sγa;θb−δicont,Π(∆ϕab) = 1{|∆ϕab|≥π/2}. Denition 8 (Eective Phase Window) . Assume experiment/simulation uses measurement grid G={(a, b)} , dene ∆ϕab and binarization rule Π(·) per above formula. Dene ∆ϕeff := ess inf (a,b)∈G |∆ϕab|. When bounded additive noise ε exists with |ε| ≤ ϵ , adopt threshold condition ∆ϕeff >π 2+ 2ϵ ; accordingly obtain Theorem 5.1's misclassication rate and sample complexity estimate. Hypothesis (independence and sub-Gaussian) Measurement samples {c ∆ϕ(n) ab }N n=1 independent, Ec ∆ϕ(n) ab = ∆ϕab , sub-Gaussian with proxy variance σ2 . Theorem 9 (5.1: Error Bound and Sample Complexity for Majority Voting) . Assume measurement samples {c ∆ϕ(n) ab }N n=1 mutually independent, Ec ∆ϕ(n) ab = ∆ϕab , sub-Gaussian with proxy variance σ2 ; with bounded additive bias |ε| ≤ ϵ . Denote m:= ∆ϕeff −π 2−2ϵ > 0, q := P|c ∆ϕ(n) ab |<π 2. Then q≤2 exp−m2 2σ2,P( majority voting misjudgment )≤exp−2N1 2−q2. Given target error δ∈(0,1) , sucient condition is N≥log(1/δ) 21 2−2e−m2/(2σ2)2, requiring m>σ√2 log 4 ensuring q < 1 2 for majority voting convergence. If oversampling correlation exists, replace N in above formula with eective sample number Neff . Proposition 10 (5.2: Dealiasing and Secondary Evidence Fusion) . For multiple crossings or nearthreshold masking: (i) Adopt multi-window sliding and anchor continuity strategy; (ii) Fuse group delay double-peak merging, conrming crossing only when both ngerprints synchronize; (iii) When crosstalk occurs, add redundant columns nearly orthogonal to existing sensitivity, recalculate Gram criterion until full rank. 6 J -Unitary Robustness: Kren Angle, Polarization Homotopy, and Threshold Function Kren angle and angle gap : Assume ⟨ψj(τ), Jψj(τ)⟩ = 0 (non-neutral eigenstate), otherwise κj undened, and that parameter point viewed as robust domain boundary and excluded. Dene 4
κj(τ) = Im ⟨ψj(τ), J S−1(∂τS)ψj(τ)⟩ ⟨ψj(τ), J ψj(τ)⟩, consistent with ∂τϕj in unitary limit J=I , used as phase slope . Angle gap dened as η:= min jinf τdistϕj(τ), π + 2πZ∈(0, π]. Near J -unitary there exist c±(ε)→1 making c−|∂τϕj| ≤ |κj| ≤ c+|∂τϕj| . Note: κj only as slope control term, not participating in η denition . Lemma 11 (6.1: Estimate from (S†JS −J) to (K−K♯) ) . Assume S(τ) pointwise invertible along considered parameter domain, with sup τ|S(τ)|<∞,sup τ|S(τ)−1|<∞,|S†JS −J| ≤ ε, β = inf τσmin(I+ iK(τ)) >0. Then constant C=Cβ, sup |S|,sup |S−1| exists making |K−K♯| ≤ C ε. Proof essentials : Use Fréchet dierential of Cayley inverse map K=−i(I+S)−1(I−S) with J -conjugation and bounded multiplier inequality. Construction 6.2 (polarization homotopy) Let Kt= (1 −t)K+t1 2(K+K♯), St= (I−iKt)(I+ iKt)−1, t ∈[0,1]. By Lemma 6.1 and Neumann lemma obtain σminI+ iKt(τ)≥β−t 2C ε, thus when ε < 2β/C , (I+iKt) invertible throughout t∈[0,1] , St well-dened. In near J -unitary calibration, constant α > 0 exists (depending on |S| , |S−1| , β ) making ε0(η, β) := min 2β C, α sin2η 2 feasible upper bound : when ∥S†JS −J∥ ≤ ε<ε0(η, β) with η > 0 , homotopy {St} doesn't intersect D , with Cayley denominator invertible throughout. Theorem 12 (6.3: Homotopy Robustness) . If homotopy {St} satisfying above formula exists without intersecting D throughout, then ν√det S⟲ equals unitary limit value. Square root asymptotics (engineering ngerprint) : Dominant branching 2×2 eective subspace yields arg det S(t) = arg det S(tc)±arctanκ1/2|t−tc|1/2+O|t−tc|3/2, group delay exhibits symmetric double-peak merging, peak separation ∆ω=Cp|t−tc|+O|t− tc|3/2 . Higher-order roots (EP order >2 ) mod-two equivalent to square root. 5
7 Floquet-SSN: Phase-Type Band-Edge Index, Truncation and Gauge Independence Denition 13 (7.1: Phase-Type Index) . Truncate sideband to |n| ≤ N obtaining nite-dimensional S(N) F(ω) , dene ν(N) F= expi 2Zπ/T −π/T ∂ωarg det S(N) F(ω) dω∈ {±1}. Equivalently, ν(N) F= expi 2Zπ/T −π/T Im ∂ωlog det S(N) F(ω) dω. Theorem 14 (7.2: Truncation Independence: Norm/HS Version) . If S(N) F→SF in operator norm or HilbertSchmidt topology, with endpoints ω=±π/T having no N -migrating branching, then N∗ exists making ν(N) F stable for N≥N∗ ; dene νF=ν(N∗) F . In HilbertSchmidt scenario , replace det dierential with Koplienko spectral shift and det2 derivative recipe, combined with Appendix F mod-two consistency, obtaining same νF . Strong convergence alone insucient to ensure det2 and second-order trace formula well-denedness, thus not included in theorem premise. Lemma 15 (7.3: Gauge Independence) . If SF(ω)7→ UL(ω)SF(ω)UR(ω) where UL,R continuous with |det UL,R|= 1 , satisfying band-edge gluing condition [arg det UL+ arg det UR]π/T −π/T ∈4πZ, then Zπ/T −π/T ∂ωarg det SF(ω) dω mod-two value invariant. Theorem 16 (7.4: Band-Edge Equivalence) . If endpoints satisfy square root local model with Theorem 7.2 holding, then νF= (−1)I2[−π/T,π/T ],DF. Failure mode 7.5 (detection and fault tolerance threshold) When truncation induces endpoint pseudo-branching, monitor min ω∈{±π/T}σmin I−CS(N) ii (ω)≥δF, requiring ν(N) F=ν(N+1) F=ν(N+2) F continuous three-order consistency to judge stable. 6
8 Prototype and SOP 8.1 Two equivalent paths for single crossing : (i) Complex parameter small loop: λ circles Jost zero once in complex plane; (ii) Real parameter traverse + frequency domain readout: Real parameter traverses D , select single branch in frequency domain using anchor continuity. Both homotopy equivalent. Along any closed loop from complex parameter small loop or real parameter traverse + return closure, have Id arg det S=±2π, expi 2Id arg det S=−1, fully consistent with 3 half-phasespectral-ow parity. 8.2 Two-port couplermicroringgain prototype (simulatable) : Coupler C(κ) = √1−κ2iκ iκ√1−κ2,C(ω, t) = ρeiϕ(ω,t). Eective scattering (Schur-closure) S⟲=See +SeiI−CSii−1CSie. In critical neighborhood of CSii →I falls back to 8.1 square root model, directly reproducing ∆φ=π and group delay double-peak merging. 8.3 SOP and criteria : Port de-embedding sweep feedback crossing D use ∆ϕeff > π/2+2ϵ and double-peak merging as passing condition; triple ngerprint asynchrony vetoes causal chain, returning to column controllability procedure for redundant column addition or frequency window reselection. 9 Readout and WignerSmith Unied Calibration ∂ωlog det S= trS−1∂ωS, ∂ωarg det S= Im trS−1∂ωS. In unitary case let Q(ω) = −iS†∂ωS , then ∂ωarg det S= tr Q(ω) . In J -unitary case can also write ∂ωarg det S= Im tr(S♯∂ωS) . 10 Conclusion This paper rigorizes half-phasespectral-shiftspectral-owintersection four-fold equivalence via bridging lemma ; ensures star-product interconnection discriminant transverse disjoint union and Z2 combinatorial law via quantitative structural lemma ; guarantees binarized projection reproducibility via concentration inequality ; characterizes near J -unitary robust domain and threshold via Kren angle and polarization homotopy ; closes band-edge topological readout chain via phase-type Floquet index and truncation/gauge independence theorems . Combined with minimal prototype and SOP, provides programmable implementation and counterfactual verication for closed-loop self-consistency ⇒ square-root criticality ⇒ double Riemann sheet ⇒Z2 half-phase. 7
References (Selected) [1] R. Redheer, On a Certain Linear Fractional Transformation, Pacic J. Math. , 9 (1959) 871 893. [2] J. Gough, M. R. James, The Series Product and Its Application to Quantum Feedforward and Feedback Networks, IEEE TAC , 54 (2009) 25302544. [3] B. Simon, Trace Ideals and Their Applications , 2nd ed., AMS (2005). [4] M. Sh. Birman, M. G. Kren, On the Theory of Wave and Scattering Operators, Sov. Math. Dokl. , 3 (1962) 740744. [5] L. Koplienko, Trace Formula for Perturbations of Class S2 , Sb. Math. , 122 (1983) 457486. [6] E. P. Wigner, Lower Limit for the Energy Derivative of the Scattering Phase Shift, Phys. Rev. , 98 (1955) 145147; F. T. Smith, Lifetime Matrix in Collision Theory, Phys. Rev. , 118 (1960) 349356. [7] T. Ya. Azizov, I. S. Iokhvidov, Linear Operators in Spaces with an Indenite Metric , Wiley (1989). [8] D. Z. Arov, H. Dym, J -Contractive Matrix-Valued Functions and Related Topics , CUP (2008). [9] I. C. Fulga, F. Hassler, A. R. Akhmerov, Scattering Formula for the Topological Quantum Number, Phys. Rev. B , 85 (2012) 165409. [10] M. S. Rudner, N. H. Lindner, E. Berg, M. Levin, Anomalous Edge States..., Phys. Rev. X , 3 (2013) 031005. A Notation and Regularization Notation : J (Kren metric), S♯=J−1S†J ; S1/S2 (trace-class/HS); det⋆ (nite-dimensional take det , HS take det2 ); D, DF (discriminant/band-edge discriminant); Λ , Πτ , η , Q=−iS†∂ωS , ν√det S⟲ , νF . Calibration : Main text adopts S1 . HS case stabilizes with det2 ; four-fold equivalence and νF mod-two value independent of det /det2 choice (see Appendix F). B CoveringLifting and Z2 Reduction Square covering p:z7→ z2 corresponds to multiplication by two in cohomology: s:X◦→U(1) exists making s2= det S⟲ if and only if [det S⟲]∈2H1(X◦;Z) . Its Z2 reduction is this paper's global half-phase invariant. C Square Root Puiseux Asymptotics and Error For 2×2 eective subblock M(t) with ∆(t)≈∆′(tc)(t−tc) , Cayley mapping to S(t)=(I−iM)(I+ iM)−1 has leading term ±arctanκ1/2|t−tc|1/2+O|t−tc|3/2, group delay exhibits symmetric double-peak merging, peak separation ∆ω=Cp|t−tc|+O|t− tc|3/2 . Substituting into 5's ∆ϕeff yields sample complexity estimate. 8
D Target-to-Device Execution Checklist and ℓ Open-loop calibration and de-embedding choose W and step size compute Sθb(ω) = ∂θbarg det S(ω) integrating into M obtain Π(M) via π/2±τ checking rank solve Π(M)x=ℓ selecting columns trigger column-by-column with ∆φ=π , double-peak merging as stop counterfactual verication and archive. ℓ= (1 −ν⋆)/2∈ {0,1}m ( ν⋆= +1 7→ 0 , ν⋆=−17→ 1 ). E Kren Angle and Homotopy Threshold under J -Unitary Assume S†JS =J , denote X=S−1˙ S . By dierentiation X♯=−X ( J -skew-Hermitian). For (λj= eiθj, vj) : ˙ θj=Im ⟨vj, JX vj⟩ v† jJvj ,κj=Im ⟨vj, JX vj⟩ v† jJvj . From above two formulas pointwise obtain κj=˙ θj , thus |˙ θ1−˙ θ2|=|κ1−κ2|. By Lemma 6.1 obtain ∥K−K♯∥ ≤ C ε . Take Kt= (1 −t)K+t(K+K♯)/2 , St= (I−iKt)(I+ iKt)−1 . By Neumann lemma obtain σmin(I+iKt)≥β−t 2C ε , thus when ε < 2β/C , St well-dened. If ∥S†JS −J∥ ≤ ε with η > 0 , constant α > 0 exists making ε0(η, β) = min{2β/C, α sin2(η/2)} feasible upper bound, uniformly ensuring Cayley denominator invertibility and discriminant noncrossing. F Regularization Independence (Unied Proposition) Proposition 17 (F.1: det /det2 Mod-Two Consistency) . Assume along closed path γ almost everywhere S⟲ unitary. If S⟲−I∈S1 then expiIγ 1 2∂log det S⟲= (−1)Sf−1= (−1)I2. If only S⟲−I∈S2 , take S1 approximation family S⟲ ϵ→S⟲ in HS topology, dene half-phase via det2 , then lim ϵ→0expiIγ 1 2∂log det S⟲ ϵ= expiIγ 1 2∂log det 2S⟲, with both sides' mod-two value consistent with Sf−1 , I2 . G Floquet Truncation, Convergence, and Failure Mode Truncate SF sideband to |m| ≤ M obtaining S(M) F . If P|m|>M ∥Km∥ → 0 ( operator norm or HS convergence; this condition implies operator norm convergence ), with endpoints having no M -migrating branching, then supω∥S(M+1) F−S(M) F∥ → 0 , M0 exists making ν(M) F stable for M≥M0 . Detection quantities: endpoint singular value threshold δF and plateau stability criterion ( ν(M) F=ν(M+1) F=ν(M+2) F ). When abnormal drift occurs increase M or reduce coupling bandwidth to avoid pseudo-branching. 9