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Spectral response of positive recurrences under memory-filtered balanced coefficient perturbations

Jul 19, 2026Research noteW. Schulz

A research note. Status: main theorem numerically confirmed (see verify_theorem.py and FINDINGS.md); proof architecture below is a skeleton, not an audited proof; novelty asserted only as "not located," not established.

Alternative accessible title: When Memory Accelerates Recurrence Growth: A Spectral Response Theorem.


1. The model

Two coupled recursions. A driving memory process (AR(1) on the forcing):

dn+1=adn+εqn,0a<1,d_{n+1} = a\,d_n + \varepsilon\,q_n, \qquad 0 \le a < 1,

and a positive companion recurrence whose coefficients it perturbs:

xn+1=(A+dn)xn+(Bdn)xn1,A,B>0.x_{n+1} = (A + d_n)\,x_n + (B - d_n)\,x_{n-1}, \qquad A, B > 0.

The perturbation is special. Written on the coefficient pair,

(A,B)    (A+dn,  Bdn),(A, B) \;\longmapsto\; (A + d_n,\; B - d_n),

it adds exactly what it subtracts:

(A+dn)+(Bdn)=A+B(conserved for every n).(A + d_n) + (B - d_n) = A + B \quad\text{(conserved for every } n).

The environment never changes the total coefficient weight; it only transfers influence between the present state xnx_n and the inherited state xn1x_{n-1}. This is the balanced coefficient transfer, and it is what makes the model distinct from ordinary additive off-diagonal disorder.

Transfer-matrix form

(xn+1xn)=Mn(xnxn1),Mn=(A+dnBdn10)=(AB10)+dn(1100).\begin{pmatrix} x_{n+1} \\ x_n \end{pmatrix} = M_n \begin{pmatrix} x_n \\ x_{n-1} \end{pmatrix}, \qquad M_n = \begin{pmatrix} A+d_n & B-d_n \\ 1 & 0 \end{pmatrix} = \begin{pmatrix} A & B \\ 1 & 0 \end{pmatrix} + d_n \begin{pmatrix} 1 & -1 \\ 0 & 0 \end{pmatrix}.

The perturbation direction is a rank-one, coefficient-conserving update of a companion matrix. Note detMn=(Bdn)\det M_n = -(B - d_n) fluctuates with the forcing — the cocycle is not naturally SL(2,R)\mathrm{SL}(2,\mathbb{R}), so the Lyapunov exponent carries a determinant/scale contribution that the usual normalized localization cocycles hide. The derivation below works directly with the positive growth of xnx_n rather than a determinant-one projective cocycle.

Constants

λ=A+A2+4B2(dominant root of t2=At+B),β=Bλ2.\lambda = \frac{A + \sqrt{A^2 + 4B}}{2} \quad(\text{dominant root of } t^2 = At + B), \qquad \beta = \frac{B}{\lambda^2}.

At ε=0\varepsilon = 0 the deterministic recurrence grows like λn\lambda^n, so the Lyapunov exponent is Λ(0)=logλ\Lambda(0) = \log\lambda.


2. Main theorem

Assumptions. qn=qTnq_n = q\circ T^n is a bounded, stationary, mean-zero forcing over an ergodic TT; σq\sigma_q is its spectral (power) measure; and ε\varepsilon is small enough that positivity holds, A+dn>0A + d_n > 0 and Bdn>0B - d_n > 0.

Claim.

  Λ(ε)=logλ+ε2ππWa,λ,β(ω)dσq(ω)+O(ε3),Λ(0)=0,  \boxed{\; \Lambda(\varepsilon) = \log\lambda + \varepsilon^2 \int_{-\pi}^{\pi} W_{a,\lambda,\beta}(\omega)\, d\sigma_q(\omega) + O(\varepsilon^3), \qquad \Lambda'(0) = 0, \;}

with the response kernel

Wa,λ,β(ω)=(λ1)[2cosω+β(λ+1)λ+1]2λ4(1+β)(1+β2+2βcosω)(1+a22acosω).W_{a,\lambda,\beta}(\omega) = \frac{(\lambda-1)\,\big[\,2\cos\omega + \beta(\lambda+1) - \lambda + 1\,\big]} {2\lambda^4\,(1+\beta)\,(1+\beta^2+2\beta\cos\omega)\,(1+a^2-2a\cos\omega)}.

The linear term vanishes because centered forcing makes the first variation mean-zero (Lemma 6); the leading effect is second order.

The factorization — the real content

Wa,λ,β(ω)=11+a22acosωMa(ω)  — memory filter(λ1)[2cosω+β(λ+1)λ+1]2λ4(1+β)(1+β2+2βcosω)Pλ,β(ω)  — projective geometry.W_{a,\lambda,\beta}(\omega) = \underbrace{\frac{1}{1+a^2-2a\cos\omega}}_{\displaystyle M_a(\omega)\;\text{— memory filter}} \cdot \underbrace{\frac{(\lambda-1)\,[\,2\cos\omega + \beta(\lambda+1) - \lambda + 1\,]}{2\lambda^4(1+\beta)(1+\beta^2+2\beta\cos\omega)}}_{\displaystyle P_{\lambda,\beta}(\omega)\;\text{— projective geometry}}.

MaM_a is exactly the power response of a one-pole (AR(1)) filter; it is everywhere positive and monotone in ω|\omega|. It contains all the aa-dependence, so the memory parameter cannot move the sign — it only reweights how strongly each frequency is felt.

Pλ,βP_{\lambda,\beta} carries the sign. Its numerator is linear in cosω\cos\omega, so it crosses zero at most once on [0,π][0,\pi]. Hence:

Memory controls strength; recurrence geometry controls sign.

This is sharper than the standard "colored noise changes a Lyapunov exponent": here the what-frequencies-help question and the how-much question separate cleanly into two factors.


3. Exact sub-results

3.1 Frequency transition (fixed recurrence)

For λ>1\lambda > 1 the response changes sign where the PP-numerator vanishes:

  cosωc=λ1β(λ+1)2.  \boxed{\;\cos\omega_c = \frac{\lambda - 1 - \beta(\lambda+1)}{2}.\;}
  • If cosωc(1,1)\cos\omega_c \in (-1,1) (Regime I, interior transition): low frequencies ω<ωc|\omega|<\omega_c enhance growth, high frequencies ω>ωc|\omega|>\omega_c suppress it.
  • If cosωc[1,1]\cos\omega_c \notin [-1,1] (Regime II): the kernel has one sign across all physical frequencies.
  • λ=1\lambda = 1 (Regime III, critical): see 3.2.

The threshold is independent of the memory parameter aa — confirmed to <103<10^{-3} rad in simulation for a=0.2a = 0.2 and a=0.6a = 0.6 (test T4).

3.2 The exact conservation anchor (A+B=1A + B = 1)

λ=1    A+B=1\lambda = 1 \iff A + B = 1. Because the transfer is balanced,

Fd(1)=(A+d)+(Bd)=1for every d,F_{d}(1) = (A + d) + (B - d) = 1 \quad\text{for every } d,

so the ratio rn=xn/xn11r_n = x_n / x_{n-1} \equiv 1 is an exact invariant for every admissible forcing sequence — not just to second order. The unit-growth state is protected nonperturbatively:

  A+B=1    Λ0 on the r1 branch, for all forcing.  \boxed{\; A + B = 1 \implies \Lambda \equiv 0 \text{ on the } r\equiv 1 \text{ branch, for all forcing.} \;}

This is why the kernel carries the factor (λ1)(\lambda - 1): at λ=1\lambda = 1 the whole second-order response vanishes identically.

3.3 Fibonacci specialization (A=B=1A = B = 1)

λ=φ=1+52,β=φ2.\lambda = \varphi = \tfrac{1+\sqrt5}{2}, \qquad \beta = \varphi^{-2}.

Sign-change frequency:

  cosωc=12φ20.1910    ωc1.7630 rad101.1.  \boxed{\;\cos\omega_c = -\frac{1}{2\varphi^2} \approx -0.1910 \;\Longrightarrow\; \omega_c \approx 1.7630\ \text{rad} \approx 101.1^\circ.\;}

So low/medium frequencies accelerate Fibonacci growth (2nd order); fast oscillations suppress it. For spectrally flat (white) forcing the integrated response changes sign at a memory threshold:

  ac=13φ0.2060.  \boxed{\; a_c = \frac{1}{3\varphi} \approx 0.2060. \;}

Below aca_c the memory is too weak to overcome the harmful high-frequency mass; above it, the low-frequency emphasis of the memory filter makes the net response positive. Both constants are confirmed: the closed-form Wdω\int W\,d\omega has its root at 0.206010.20601, and simulated white-noise C(a)C(a) crosses zero between a=0.1a=0.1 (C<0C<0) and a=0.35a=0.35 (C>0C>0), passing through 0\approx 0 at aca_c (test T5).


4. Proof architecture (skeleton)

Work with the ratio rn=xn/xn1r_n = x_n/x_{n-1}, which follows the Riccati/Möbius map

rn+1=Fdn(rn)=(A+dn)+Bdnrn,Λ=E[logr].r_{n+1} = F_{d_n}(r_n) = (A + d_n) + \frac{B - d_n}{r_n}, \qquad \Lambda = \mathbb{E}[\log r_\infty].
  • Lemma 1 (bounded stationary memory). Dε(y)=εj0ajq(T1jy)D_\varepsilon(y) = \varepsilon\sum_{j\ge0} a^j q(T^{-1-j}y) solves Dε(Ty)=aDε(y)+εq(y)D_\varepsilon(Ty)=aD_\varepsilon(y)+\varepsilon q(y) with Dεεq/(1a)\|D_\varepsilon\|_\infty \le \varepsilon\|q\|_\infty/(1-a). Controls positivity.
  • Lemma 2 (absorbing interval). For dδ<min(A,B)|d|\le\delta<\min(A,B), all positive ratio trajectories enter a common compact interval.
  • Lemma 3 (two-step contraction). FdF_d reverses order, but Fd2Fd1F_{d_2}\circ F_{d_1} preserves it with derivative (Bd1)(Bd2)((A+d1)r+Bd1)2<1\frac{(B-d_1)(B-d_2)}{((A+d_1)r + B-d_1)^2} < 1 on the absorbing interval for small δ\delta.
  • Lemma 4 (unique invariant graph). The two-step graph transform is a contraction ⇒ unique RεR_\varepsilon with Rε(Ty)=FDε(y)(Rε(y))R_\varepsilon(Ty)=F_{D_\varepsilon(y)}(R_\varepsilon(y)); every positive initial ratio synchronizes exponentially.
  • Lemma 5 (smoothness). Uniform contraction + analyticity of FdF_d away from r=0r=0εRε\varepsilon\mapsto R_\varepsilon is C3C^3 near 00.
  • Lemma 6 (first variation). Expanding Rε=λ+εW+ε2V+O(ε3)R_\varepsilon = \lambda + \varepsilon W + \varepsilon^2 V + O(\varepsilon^3), WT=βW+γZW\circ T = -\beta W + \gamma Z with γ=11/λ\gamma = 1 - 1/\lambda; centered forcing gives E[W]=0\mathbb{E}[W]=0, hence Λ(0)=0\Lambda'(0)=0.
  • Lemma 7 (second variation). VT=βV+ZW/λ2+BW2/λ3V\circ T = -\beta V + ZW/\lambda^2 + BW^2/\lambda^3; solving the linear filters for Z,WZ,W and applying the spectral theorem for stationary processes yields the kernel Wa,λ,βW_{a,\lambda,\beta}.

Caveat that must be stated in the theorem. The constants are not uniform as a1a\to1^-: since Dεεq/(1a)\|D_\varepsilon\|_\infty \le \varepsilon\|q\|_\infty/(1-a), the admissible perturbation scales like ε1a|\varepsilon| \lesssim 1-a. The theorem must read "for every fixed a<1a<1 there exists ε0(a)>0\varepsilon_0(a)>0," not one ε0\varepsilon_0 for all a[0,1)a\in[0,1).


5. Relation to known work (threat assessment)

Established, not claimed here:

  • random / weakly-disordered transfer matrices and perturbative Lyapunov exponents;
  • correlated diagonal and off-diagonal disorder; correlation-induced mobility edges;
  • random Fibonacci recurrences and their Riccati ratio maps;
  • regularity/response of Lyapunov exponents under perturbation;
  • general linear-response machinery for skew products with contracting fibers.

Not located in targeted searches (⇒ candidate novelty, not proven): the specific balanced-transfer model (A+dn,Bdn)(A+d_n, B-d_n) with an external AR(1) memory parameter, its closed-form second-order kernel, the clean MaPM_a\cdot P factorization (sign independent of memory), and the Fibonacci constants cosωc=1/2φ2\cos\omega_c = -1/2\varphi^2, ac=1/3φa_c = 1/3\varphi.

Verdict after literature review (deflated). The real check was done and the general result is established prior art. The form "weakly/randomly perturbed 2×2 recurrence ⇒ Λ(ε)=Λ₀+ε²·(spectral integral)+O(ε³), Λ′(0)=0, kernel integrated against the forcing's spectral density" is owned by weak-noise Lyapunov expansions (Arnold, Papanicolaou & Wihstutz, SIAM J. Appl. Math. 46 (1986) 427–450; and "products of random 2×2 matrices close to the identity," arXiv:1208.6430) and by weak-disorder Lyapunov/localization theory (Thouless-type γ, correlated/colored disorder feeding a power spectrum into the kernel). The AR(1) memory M_a is just a Lorentzian noise spectrum plugged into that known formula. The specific balanced-transfer direction and the golden-ratio constants appear unpublished in this exact form, but they fall out mechanically — the equivalent of evaluating a known general integral for a particular integrand. Honest classification: a new worked example inside a fully established framework, not a new theorem and not a new field. This supersedes the earlier "original special theorem" self-assessment. Full citations and options in FINDINGS-spectral-response.md.

6. What is verified vs. open

Verified numerically (verify_theorem.py, T1–T5 all PASS): the baseline logφ\log\varphi; clean ε2\varepsilon^2 scaling with Λ(0)=0\Lambda'(0)=0; kernel shape match to kWa(ω)k\cdot W_a(\omega) at shape-correlation 1.00001.0000 for two memory values; aa-independence of ωc\omega_c; the flat-forcing threshold ac=1/3φa_c=1/3\varphi (both formula-self-consistent and simulation-confirmed).

Open: audited proof of Lemmas 1–7; the nn-th-order generalization (transfer across many past states); nonlinear updates; and the practical applications in docs/applications-directions.md.

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