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Nonlinear Phase Stabilization in Quantum Information Systems: An LA-ODR Framework with Temporal Susceptibility Feedback

Andriy V Lemeshko, Isamu Ohnishi

Published Apr 19, 2026• 0 citations
Publisher

Abstract

ABSTRACT The scalability of Noisy Intermediate-Scale Quantum (NISQ) devices [21] remains fundamentally limited by decoherence, which conventional dynamical decoupling [25] and quantum error correction [26, 28] only partially mitigate. This paper presents a transition from passive noise suppression to active dynamical stabilization through controlled modulation of the effective state-space metric. Within the Lie-algebraic renormalization (LA-ODR) framework [5, 6, 7], we introduce the Temporal Phase-Locked Loop (TPLL) — an active feedback controller that drives the temporal susceptibility χ_τ toward the globally stable fixed point χ_τ* = λ_nat/(λ_ctrl + λ_nat) via the Kyiv–Ohnishi hybrid flow: dχ_τ/dt = −α · Γ₀ · (χ_τ)^(β+1) − λ_ctrl · χ_τ + λ_nat · (1 − χ_τ) Numerical simulations (illustrative) demonstrate the emergence of metastable coherence plateaus extending coherence times from ~100 µs to ~1.5 ms under realistic hardware benchmarks (FPGA latency Δt < 500 ns). The model predicts two experimentally distinguishable signatures: (i) Phase Inertia — non-exponential initial coherence suppression; and (ii) Avalanche Collapse — a second-order phase transition at χ_τ > χ_crit. These signatures distinguish the TPLL regime from standard Lindblad decay and passive discrete time crystals. Keywords: nonlinear phase stabilization; temporal susceptibility; LA-ODR; Kyiv–Ohnishi flow; TPLL; coherence plateau; Avalanche Collapse; Phase Inertia; NISQ devices; discrete time crystals; Krylov tower invariance

DOI
10.5281/zenodo.19651032

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ABSTRACT The scalability of Noisy Intermediate-Scale Quantum (NISQ) devices [21] remains fundamentally limited by decoherence, which conventional dynamical decoupling [25] and quantum error correction [26, 28] only partially mitigate. This paper presents a transition from passive noise suppression to active dynamical stabilization through controlled modulation of the effective state-space metric. Within the Lie-algebraic renormalization (LA-ODR) framework [5, 6, 7], we introduce the Temporal Phase-Locked Loop (TPLL) — an active feedback controller that drives the temporal susceptibility χ_τ toward the globally stable fixed point χ_τ* = λ_nat/(λ_ctrl + λ_nat) via the Kyiv–Ohnishi hybrid flow: dχ_τ/dt = −α · Γ₀ · (χ_τ)^(β+1) − λ_ctrl · χ_τ + λ_nat · (1 − χ_τ) Numerical simulations (illustrative) demonstrate the emergence of metastable coherence plateaus extending coherence times from ~100 µs to ~1.5 ms under realistic hardware benchmarks (FPGA latency Δt < 500 ns). The model predicts two experimentally distinguishable signatures: (i) Phase Inertia — non-exponential initial coherence suppression; and (ii) Avalanche Collapse — a second-order phase transition at χ_τ > χ_crit. These signatures distinguish the TPLL regime from standard Lindblad decay and passive discrete time crystals. Keywords: nonlinear phase stabilization; temporal susceptibility; LA-ODR; Kyiv–Ohnishi flow; TPLL; coherence plateau; Avalanche Collapse; Phase Inertia; NISQ devices; discrete time crystals; Krylov tower invariance
Abstract: The scalability of Noisy Intermediate-Scale Quantum (NISQ) devices remains fundamentally limited by decoherence, which conventional dynamical decoupling and quantum error correction only partially mitigate. This paper presents a transition from passive noise suppression to active dynamical stabilization through controlled modulation of the effective state-space metric. Within the Lie-algebraic observable-dependent renormalization (LA-ODR) framework, we introduce the Temporal Phase-Locked Loop (TPLL) — an active feedback controller that drives the temporal susceptibility χ_τ toward the globally stable fixed point χ_τ* = λ_nat/(λ_ctrl + λ_nat) via the Kyiv–Ohnishi hybrid flow: dχ_τ/dt = −α·Γ₀·(χ_τ)^(β+1) − λ_ctrl·χ_τ + λ_nat·(1−χ_τ). Numerical simulations demonstrate the emergence of metastable coherence plateaus extending coherence times from ~100 µs to ~1.5 ms under realistic hardware benchmarks (FPGA latency Δt < 500 ns). Three operationally distinct zones are characterized by χ_τ thresholds, and two experimentally distinguishable signatures — Phase Inertia and Avalanche Collapse — are predicted. The TPLL is compared with dynamical decoupling, quantum error correction, and discrete time crystals, establishing complementarity rather than competition. The mathematical foundations rest on four global stability theorems via Lyapunov analysis and Chiba renormalization-group flow. Index Terms: Quantum coherence; decoherence control; temporal susceptibility; LA-ODR; Temporal Phase-Locked Loop (TPLL); Kyiv–Ohnishi flow; NISQ devices; open quantum systems; Lyapunov stability; Lie algebra; FPGA quantum control; nonlinear dynamics.
Abstract: The scalability of Noisy Intermediate-Scale Quantum (NISQ) devices remains fundamentally limited by stochastic decoherence, which traditional passive shielding and resource-heavy quantum error correction (QEC) struggle to overcome. Here, we propose a paradigm shift from passive noise mitigation to active internal phase stabilization. By integrating the Lie-algebraic renormalization (LA-ODR) framework with a dynamic model of temporal susceptibility (χ_τ), we derive a nonlinear control law for quantum coherence. We demonstrate that decoherence can be treated as a deterministic dynamical process governed by the feedback equation dχ_τ / dt = −α · Γ_τ · χ_τ + λ · (1 − χ_τ). Our numerical simulations confirm the formation of metastable coherence plateaus, where the effective qubit lifetime is extended significantly beyond the standard Lindbladian limit (e.g., from 100 µs to 1.5 ms in transmon-based models). We further specify a hardware-ready Temporal Phase-Locked Loop (TPLL) architecture, proving that with control latencies below 500 ns, active synchronization of the temporal metric becomes feasible on modern FPGA-based controllers. This framework provides a path toward fault-tolerant quantum computing by enabling fidelity-by-design at the physical layer, potentially providing a substantial reduction in QEC overhead by maintaining high physical fidelity prior to logical encoding. Keywords nonlinear phase stabilization; temporal susceptibility χτ; Lie-observable-dependent renormalization (LA-ODR); fixed-point Lindbladian; quantum decoherence; active feedback control; temporal phase-locked loop (TPLL); NISQ devices; superconducting qubits; cold atom arrays
The standard theory of quantum decoherence treats the environment as an external reservoir imposing a fixed decoherence rate. We propose a fundamental reinterpretation: within the Lie-Observable-Dependent Renormalization (LA-ODR) framework, the decoherence rate Γτ = Γ₀(χτ)^β is governed by the temporal susceptibility χτ — a state-dependent order parameter of phase-ensemble desynchronization. We derive the Kyiv–Ohnishi hybrid flow dχτ/dt = -αΓ₀(χτ)^(β+1) - λ_ctrlχτ + λ_nat(1-χτ), establish four theorems of global asymptotic stability via Lyapunov analysis, and prove a triple algebraic–geometric–thermodynamic correspondence at the fixed point χτ* = λ_nat/(λ_ctrl + λ_nat). The effective state-space metric dsτ² = (1-χτ)c²dt² - (1+χτ)dx² is a Riemannian analogue of the Fubini–Study metric on susceptibility space, not a physical spacetime metric. The framework provides the mathematical foundation for active coherence control in NISQ quantum devices.
We present a rigorous Lie‑algebraic realization of the temporal interpretation of quantum decoherence recently proposed by Lemeshko et al. (2026). By promoting the temporal drift δτ(t) to an observable‑dependent generator Xtime inside the dynamical Lie algebra g = Lie{ iH, Lk, L†k, Oi } we perform systematic Lie closure to extract the maximal Lie‑observable‑dependent symmetry (Lie‑ODS) subalgebra whose adjoint action leaves the entire Krylov tower of phase‑synchronization observables { Re(ac), Im(ac), a†cac } invariant. Embedding this construction into the hierarchical Lie‑observable‑dependent renormalization (LA‑ODR) flow yields a universal fixed‑point Lindbladian L˜* of remarkably small and constant dimension d* = 4–9, independent of the ultraviolet cutoff. The resulting model exactly reproduces the exponential phase‑damping law ρij(t) = ρij(0) · exp(−Γτ · t) of the original temporal picture, with the decoherence rate γ ≡ Γτ emerging as a universal fixed‑point parameter. Non‑Markovian memory effects and 1/f noise appear naturally as residual temporal correlations between successive RG scales, while complete positivity and trace preservation are rigorously maintained at every coarse‑graining step. When augmented with variational quantum minimal models (VQMM), the framework enables NISQ photonic devices to self‑optimize their own temporal synchronization in real time, achieving Bloch‑vector errors below 3.2 × 10⁻⁴. The surviving Lie‑ODS subalgebra supplies a precise open‑system analogue of Noether’s theorem for temporal symmetries and opens a direct route to topological diagnostics via cyclic multi‑information measures. This work closes the long‑standing interpretive gap between phenomenological temporal pictures and exact effective theories in the thermodynamic limit. It unifies the temporal desynchronization ansatz with the same LA‑ODR machinery previously applied to quantum frequency combs and exciton‑polariton condensation, revealing the remarkable universality of observable‑dependent renormalization. The resulting fixed‑point Lindbladian is computationally trivial yet physically complete, offering powerful new tools for noise analysis, phase stability, and quantum information processing in complex open systems. Future extensions include spatially inhomogeneous drifts, dynamical fermions, and holographic analogues of quantum gravity in open quantum systems.
Traditional Quantum Error Correction (QEC) methods maintain logical qubit states by artificially overriding native quantum dynamics [3], relying on redundancy, frequent measurements, and external feedback. This work proposes an alternative model for intrinsic quantum stabilization via gravitooscillatory phase alignment [5], [6]. We introduce the theoretical stabilizer term S(Φ) = λG 1+γΦ 2 , where long-term coherence emerges naturally from passive coupling with structured vibrational fields. To operationalize this model, we developed the STDJ algorithm-an acronym in Portuguese for Sistema Temporal de Dobra Justa ("System of Temporal Just-Fold")-a computational implementation that harmonically interpolates evolving qubit signals. Numerical simulations reveal that quantum systems governed by H = H0 + S(Φ) exhibit extended coherence times compared to conventional Hamiltonians, even under decoherence channels [1]. Measured fidelities F (t) remain above 0.99 across temporal evolution, supporting the hypothesis that coherence can be maintained via symbolic self-resonance [15]. These findings point to a paradigm where quantum robustness originates not from error negation, but from oscillatory alignment within multidimensional phase spaces. Together, the STDJ framework and the stabilizing term S(Φ) reveal a resonance-based coherence landscape with implications for scalable quantum architectures beyond error correction.