LLMs are revolutionizing science education. For any topic, you can now generate interactive explanations, adapt them in real time, and play with them until it clicks. Underrated.

LLMs are revolutionizing science education. For any topic, you can now generate interactive explanations, adapt them in real time, and play with them until it clicks. Underrated.
I just met Denis Noble at the royal institute last week and heard his fascinating short lecture on "Chemistry of Life begins with Water"
Aleksandr Mikhailovich Lyapunov (1857 – 1918)
Aleksandr Lyapunov, The general problem of the stability of motion, 1892. Lyapunov functions of an ODE are functions which decay along the flows of the ODE. The basic method to show convergence to a stationary point and its stability.
Samim.A.Winiger - 12.May.2025
Oscillatory neural networks (ONNs) hold significant promise for advanced AI, yet their complex internal dynamics impede robust design and verification. Current analytical tools often fall short in providing rigorous stability guarantees and comprehensive, interpretable insights for these systems. This paper introduces PhaseScope, a theoretical framework and computational toolkit designed to bridge this gap. PhaseScope integrates three core pillars: (1) a novel field-aware embedding theory for reconstructing high-dimensional attractors from distributed neural activity; (2) advanced spectral stability diagnostics for spatio-temporal patterns; and (3) systematic methods for active hidden-attractor exploration.
By combining these advances, PhaseScope aims to establish stronger theoretical foundations and reliable diagnostic tools for the principled design, analysis, and deployment of Oscillatory Neural Networks.
Oscillator-based networks, utilizing phase-encoding and coupled oscillatory dynamics, offer significant potential for advanced AI applications. However, a comprehensive understanding of their internal dynamics, particularly in spatially extended architectures, remains a critical challenge. While numerous powerful analytical tools exist for dynamical systems and machine learning (including operator-theoretic methods, manifold learning, and TDA, as discussed in Sec. 5.5), the application of rigorous dynamical systems tools (like state-space reconstruction and detailed stability analysis) to understand the internal workings and ensure the robustness of ONNs used in AI is still an emerging area. Current approaches, when applied in isolation or heuristically to these specialized networks, can face limitations in providing verifiable stability margins, comprehensive hidden-mode discovery, and clear paths to interpretable, robust design.
This proposal introduces PhaseScope, a theoretical framework and computational toolkit designed to address this gap by providing the necessary "microscope" to bridge functional performance with fundamental dynamical understanding. PhaseScope integrates three core components:
The overarching objective is to establish a unified methodology that moves beyond heuristic approaches, providing stronger theoretical foundations and reliable diagnostic tools for the principled design, verification, and trustworthy deployment of oscillator-based AI systems.
As machine learning researchers enthusiastic about the potential of oscillatory AI, we approach the advanced mathematics and nonlinear dynamics involved with a “beginner’s mind"—echoing Zen master Shunryu Suzuki’s insight that “in the beginner’s mind there are many possibilities, but in the expert’s there are few”. This spirit fuels our commitment to hands-on exploration, to learning by building, and critically, to making these complex systems and their sophisticated analysis more accessible to a broader range of practitioners.
PhaseScope’s key contributions to the analysis of oscillator-based neural networks include:
Neural network architectures increasingly draw inspiration from neurobiological principles, among which oscillatory dynamics and phase-based information encoding are particularly prominent. Oscillator-based neural networks offer compelling advantages for artificial intelligence tasks, including robust temporal sequence representation and efficient rhythm tracking, lending themselves to potentially more energy-efficient and dynamically rich computational models.
Despite their promise, the widespread adoption of these networks is hampered by the opaque nature of their internal dynamics. As networks are trained, they can settle into complex operational regimes. Understanding _how_ they compute or _why_ they succeed or fail often remains elusive. This “black-box” character leads to practical pain points: brittle training, unpredictable performance, undetected failure modes (hidden attractors that compromise reliability), and significant difficulties in verification and validation for critical applications.
The vision for PhaseScope is to address these critical challenges by providing a rigorous, data-driven “microscope” for the design, diagnosis, and control of oscillator-based neural networks. We aim to move the field beyond heuristic approaches towards a paradigm where the behavior of these systems can be understood and predicted with enhanced confidence and stronger theoretical backing. PhaseScope endeavors to equip researchers and engineers with tools to illuminate internal workings, enable principled design, and ensure more trustworthy AI by transforming trained oscillator networks into more transparent systems.
Ultimately, we envision PhaseScope as part of a broader framework that does for oscillator-based AI systems what PyTorch did for differentiable programming: offering an integrated, principled toolkit that translates theoretical insights into practical design and analysis tools.
The PhaseScope framework builds on dynamical systems theory, time-series analysis, and computational science, extending established methods to address the unique challenges of oscillator-based neural networks (ONNs) and their current analytical limitations.
The reconstruction of a system’s attractor from observed time series data using delay coordinates is a cornerstone of nonlinear dynamics.
Takens’ theorem (1981) provided a foundational guarantee that for a generic smooth observation \(h\) and flow \(\Phi^t\) on a compact \(d\)-dimensional manifold, the delay-coordinate map is an embedding if the embedding dimension \(m > 2d\) (Takens 1981).
"Embedology" (Sauer, Yorke & Casdagli, 1991) extended this to fractal attractors, establishing the embedding bound \(m > 2d{A}\) (where \(d{A}\) is the box-counting dimension), critical for complex attractors in neural systems (Sauer et al. 1991).
Practical limitations: While Takens’ theorem and its extensions provide a powerful theoretical foundation, their practical application is subject to important constraints. Embedding-based reconstructions are highly sensitive to measurement noise, and even moderate noise can severely degrade attractor reconstruction and parameter estimation (Casdagli et al., 1991). The amount of data required for reliable embedding increases rapidly with the effective dimensionality of the system (Eckmann & Ruelle, 1992), making high-dimensional or weakly synchronized systems especially challenging. Methods for selecting embedding parameters (such as delay and dimension) are heuristic and can be unstable in noisy or short datasets. Moreover, colored noise and certain stochastic processes can produce apparent attractor-like structures, complicating the distinction between genuine low-dimensional chaos and random dynamics (Osborne & Provenzale, 1989; Provenzale et al., 1992).
While classical embedding theory predominantly addresses scalar time series, oscillator networks generate field-valued data. Reconstructing dynamics from such data requires significant extensions.
Understanding the stability of periodic behaviors is crucial. Floquet theory provides a rigorous framework for ODEs with time-periodic coefficients (Nayfeh & Balachandran 1995, Ch. 7).
A hidden attractor is one whose basin of attraction does not intersect with small neighborhoods of equilibria, distinguishing them from “self-excited” attractors (Leonov & Kuznetsov 2013; Kuznetsov et al. 2015).
The PhaseScope framework is engineered to provide a comprehensive, multi-faceted analysis of oscillator-based neural networks. It rests upon three synergistic core pillars, each addressing a critical aspect of understanding and characterizing these complex dynamical systems. These pillars are designed to work in concert, moving from data acquisition and state-space reconstruction to stability analysis and the exhaustive mapping of all relevant dynamical regimes.
The first pillar focuses on reconstructing the system’s high-dimensional attractor from spatially distributed observations using a novel field-aware embedding theory (detailed in Section 6.2.1). This involves capturing sufficient information from selected sensor channels to represent the state of the oscillator network faithfully. Practical selection of the delay \(\tau\) and per-channel embedding dimension \(m_{ch}\) will be guided by established methods adapted for multi-channel data, such as mutual information and false near-neighbor analysis (further detailed in the EmbedExplorer module, Section 6.3.2). The goal is to produce a reliable geometric representation of the system’s dynamics, which forms the foundation for subsequent analysis by the other pillars.
The second pillar focuses on rigorously assessing the stability of periodic and spatio-temporally periodic operational modes identified within the oscillator network. Many functional states in these networks, such as those responsible for generating rhythmic patterns, maintaining clock-like oscillations, or representing entrained responses, are inherently periodic or involve repeating spatial patterns that evolve periodically in time. This pillar leverages Floquet-Bloch theory for systems with appropriate symmetries, and extends to a broader suite of spectral tools (including Lyapunov exponent analysis) for more general network structures and dynamics, as detailed in Section 6.2.3. This pillar is vital for understanding the robustness of desirable functional states. It seeks to provide well-grounded stability margins, indicating how susceptible a given operational mode is to noise, parameter drift, or input perturbations, thereby informing network design for enhanced reliability.
SpectraLab will continuously monitor the network’s proximity to critical dynamical boundaries by tracking key indicators (e.g., Lyapunov exponents nearing zero, Floquet multipliers approaching unity, or topological changes detected by TopoTrack). Recognizing that precise “edge-of-chaos” thresholds are system-dependent and a research challenge [cf. Bertschinger & Natschläger 2004], PhaseScope will provide diagnostics and alerts based on these indicators. When alerts suggest the system is nearing instability or excessive order, PhaseScope aims to facilitate (and potentially automate) cautious, iterative tuning of relevant network parameters (like global coupling or noise levels). This aims to maintain computationally rich dynamics while preventing collapse, leveraging efficient stability assessment methods (e.g., Krylov subspace techniques [cf. Lehoucq et al. 1998]) for scalability.
The third pillar is dedicated to the systematic discovery and characterization of hidden attractors. These are stable dynamical regimes whose basins of attraction do not connect to any obvious equilibria or easily found periodic orbits. Standard simulation approaches, typically initiated from random states or quiescent conditions, may entirely miss these hidden modes, which can represent latent failure states, unexpected operational capabilities, or transitions to undesirable behaviors.
PhaseScope’s Active Hidden-Attractor Exploration will employ:
The scientific importance of this pillar lies in its potential to provide a far more complete picture of a network’s dynamical landscape than is typically achieved. By actively seeking out these elusive “dark” regimes, PhaseScope aims to identify potential vulnerabilities or unexploited capabilities, contributing to the safety, robustness, and overall trustworthiness of oscillator-based AI. While comprehensively mapping all basins in high-dimensional systems can be computationally prohibitive (potentially exponential complexity), these heuristic methods aim to significantly improve discovery efficiency in practice.
The PhaseScope framework’s analytical rigor stems from adapting established mathematical principles and introducing specific theoretical advancements. These foundations underpin the methodologies in each core pillar (Section 6.1), enabling robust analysis tailored to the unique challenges of spatially extended, nonlinear oscillator networks and aiming for deeper insights.
6.2.1. Towards a “Neural Takens” Theorem: Embedding Spatially Distributed Oscillator Dynamics
The cornerstone of our Field-Aware Delay Embedding pillar is the formulation and rigorous investigation of a "Neural Takens” Theorem, tailored for spatially extended oscillator networks. This endeavor explicitly builds upon classical embedding theory, which requires certain prerequisites: the system’s dynamics must be smooth and evolve on a compact attractor, the observation function must be generic (in a Ck sense, meaning its derivatives up to order k are continuous and well-behaved), and the embedding dimension must be sufficiently high (Whitney, 1936; Takens, 1981; Sauer et al., 1991).
Building on Foundations: Classical Takens’ theorem (Takens, 1981) established that for a \(d\)-dimensional smooth attractor, a delay-coordinate map from a _generic_ scalar observation function forms an embedding if the embedding dimension \(m > 2d\). Whitney’s embedding theorem (Whitney, 1936) provides an even earlier conceptual basis, showing a \(d\)-manifold embeds in \(\mathbb{R}^{2d+1}\). Sauer et al. (1991) extended these ideas to fractal attractors. Robinson (2005) further generalized embedding concepts to infinite-dimensional systems possessing finite-dimensional attractors. Our work directly addresses the critical next step: extending these guarantees to practical, multi-channel observations from spatially distributed neural fields. This involves drawing from recent advancements in multi-channel embedding theorems (e.g., Kukavica & Robinson 2004) and embedding techniques specifically for neural fields. A central challenge, which PhaseScope aims to address, is the impact of observational and system noise (Stark et al., 2003), ensuring robust embedding under realistic conditions.
Inertial Manifold Hypothesis & Genericity in Neural Networks: A key working hypothesis is that the complex dynamics of many relevant oscillator network models (e.g., coupled Kuramoto oscillators (Kuramoto, 1984), FitzHugh-Nagumo arrays, certain classes of recurrent neural networks) effectively evolve on an \(N\)-dimensional inertial manifold \(\mathcal{M}\), despite their high nominal dimensionality (see Temam, 1997 for general background on inertial manifolds, particularly in the context of infinite-dimensional systems). Establishing or verifying conditions for the existence and finite-dimensionality of such manifolds for _trained_ oscillator networks, and clarifying how genericity conditions for embedding apply to neural oscillators with specific coupling symmetries, are important areas for detailed investigation within this framework.
The “Neural Takens” Conjecture for Multi-Channel Observations: We conjecture that a delay-coordinate map \(H_{\mathbf{P}, \tau, m_{ch}}\), constructed from \(P\) sensor channels (pointwise neuronal activity, local field potentials, or derived spatial modes \(\mathbf{y}_{k}(t)\)) with delay \(\tau\) and \(m_{ch}\) delays per channel (yielding a total embedding dimension \(m_{\text{total}} = P \times m_{ch}\)), forms an embedding of the system’s attractor \(\mathcal{A} \subset \mathcal{M}\) if \(m_{\text{total}} > 2 \dim_{B}(\mathcal{A})\). This formulation aligns with the classical \(> 2d_{A}\) requirement from Sauer et al. (1991) but explicitly leverages multiple synchronous observation streams. This approach is conceptually supported by work like Kukavica & Robinson (2004), who demonstrated that sufficiently many spatial point observations can embed a PDE’s attractor, and Robinson’s (2005) results on embedding infinite-dimensional systems using a large number of point measurements. The rigorous substantiation of this conjecture for ONNs, particularly concerning the interplay between \(P\), \(m_{ch}\), and \(\dim_{B}(\mathcal{A})\) in the context of neural field-like data and oscillator network characteristics, is a primary research goal of PhaseScope.
Spatio-Temporal Observability as a Linchpin: Crucially, the selection of sensor locations/modes \(\mathbf{P}\) is not arbitrary. It must satisfy a stringent _spatio-temporal observability condition_. This condition requires that the chosen set of sensors \(\mathbf{P}\), through their collective time-delayed measurements, can uniquely distinguish any two distinct states on the attractor \(\mathcal{A}\). Formally, this implies that the multi-channel observation function mapping states on \(\mathcal{A}\) to the sequence of measurements must be an immersion (i.e., its derivative is full rank), and for a compact attractor, this ensures an embedding (see, e.g., Guillemin & Pollack 1974 for the principle that an immersion from a compact manifold is an embedding). This moves beyond assuming a single scalar observation is _a priori_ generic in the sense of Takens (1981), instead focusing on ensuring the _chosen set_ of practically implementable sensors collectively provides sufficient information to distinguish neighboring states on the attractor. The necessity for multiple observation channels or carefully chosen single field measurements is underscored by known counterexamples in spatially extended systems (e.g., certain solutions to the complex Ginzburg-Landau equation can yield identical time series at a single spatial point, thereby failing to distinguish different spatial patterns). PhaseScope thus emphasizes multi-channel strategies designed to meet this observability demand, with robustness to noise being a key criterion for validating these strategies.
Addressing Genericity and Dimensionality: While the \(> 2 \dim_{B}(\mathcal{A})\) bound is standard for generic delay embeddings, its practical application to potentially very high-dimensional attractors in large networks necessitates careful consideration. Our investigation will link the required \(P \times m_{ch}\) to the complexity of _functional_ dynamics rather than merely network size, and explore how network architecture (e.g., sparse vs. dense connectivity, local vs. global coupling) influences \(\dim_{B}(\mathcal{A})\) and the satisfaction of observability conditions. Verifying that our proposed sensor configurations and the resulting observation functions meet the necessary genericity conditions for specific network architectures and sensor types will be a key research thrust, potentially leading to structural properties of the network rather than relying on abstract mathematical genericity alone.
The proof strategy for such a “Neural Takens” theorem will involve adapting techniques from differential topology and geometric measure theory, potentially including arguments related to the transversality of intersections for multi-sheeted embeddings arising from multi-channel observations, to specifically address the structured nature of \(H{\mathbf{P}, \tau, m{ch}}\) and the properties of attractors in common neural oscillator models.
6.2.2. Optimal Sensor Placement via Observability Gramian Analysis & Refinement
The practical utility of the “Neural Takens” theorem critically depends on selecting an effective, and ideally minimal, set of sensors. PhaseScope will develop a principled, adaptive strategy for sensor placement:
Linearized Observability as a Starting Point: We will initially leverage the Observability Gramian (\(\mathcal{W}_o\)) (see, e.g., Kailath 1980), computed from the linearized network dynamics around representative operational states (e.g., specific periodic orbits, or averaged dynamics over a typical trajectory segment if the system is chaotic). The goal is to select sensor locations/modes that maximize a robust metric of \(\mathcal{W}_o\) (e.g., its smallest eigenvalue, or a condition number related metric), thus ensuring local observability of all dynamical modes.
Computational Considerations: While powerful, the computation of the full Observability Gramian can scale as \(N^k\) or higher for networks of \(N\) oscillators if all cross-correlations are considered naively. A key aspect of SensorDesigner will be to investigate and implement computationally efficient approximations, explore methods leveraging network sparsity or structural properties (potentially inspired by methods for scalable Gramian computation, e.g., Obermeyer et al. 2018), and iterative refinement schemes to make optimal sensor placement tractable for large-scale networks.
Addressing Nonlinearity and Multiple Regimes:
This layered approach to sensor selection aims to provide data that is rich enough for successful embedding, balancing theoretical rigor with computational feasibility.
6.2.3. Floquet–Bloch and Alternative Spectral Stability Analyses for Structured and Disordered Networks
PhaseScope’s stability analysis for spatio-temporal patterns will employ a formal Floquet-Bloch framework. It is crucial to acknowledge from the outset the foundational assumptions: classical Floquet theory applies to systems linearized around a strictly time-periodic orbit, yielding Floquet multipliers whose magnitudes determine stability (Nayfeh & Balachandran, 1995). Bloch’s theorem applies to systems with perfect spatial periodicity (e.g., crystal lattices), allowing solutions to be expressed as Bloch waves indexed by a wavevector \(\mathbf{q}\) (Rabinowitz, 2000). The combination, Floquet-Bloch analysis, is therefore rigorously applicable to determine the stability of spatio-temporal patterns that are periodic in both time and space within a perfectly regular lattice structure. The specific application of Floquet theory to neural oscillators (e.g., Rugh et al. 2015) and the challenges of extending Floquet-Bloch analysis to complex, non-ideal network structures (e.g., Pecora & Carroll 1998, particularly regarding the Master Stability Function for networked systems; Strogatz 2000 as a general textbook reference for disordered systems) are active areas of research that PhaseScope aims to contribute to and build upon.
Foundation & Ideal Cases: For network states \(\phi(\mathbf{x}_j, t)\) periodic in time \(T\) on an ideal spatial grid, linearization around a spatio-temporal orbit \(\phi_0(\mathbf{x}_j, t)\) yields a time-periodic linear system. If the grid possesses discrete translational symmetry, the Bloch transformation decouples this system into independent Floquet problems for each wavevector \(\mathbf{q}\) in the Brillouin zone. The resulting spatio-temporal Floquet multipliers \(\rho(\mathbf{q})\) (or exponents \(\lambda(\mathbf{q})\)) determine stability. This provides elegant analytical modes and a clear band structure for stability.
Relationship to Master Stability Function (MSF): For networks of coupled identical oscillators exhibiting a synchronized periodic state, the Master Stability Function (MSF) framework (Pecora & Carroll, 1998; Barahona & Pecora, 2002) provides a powerful and widely adopted method. The MSF approach decouples stability analysis along the eigenmodes of the network’s coupling matrix, effectively performing a Floquet analysis for each transverse mode. PhaseScope builds upon these foundational ideas, aiming to extend stability diagnostics to more complex spatio-temporal patterns (beyond simple synchrony) and to address non-identical oscillators or less regular structures where the classical MSF assumptions might be too restrictive.
Addressing Architectural Realities: Heterogeneity, Disorder, and Non-Periodic Dynamics:
Limitations and Adaptations: Real oscillator networks often deviate from ideal periodicity due to parameter mismatches, irregular connectivity (disorder), or by settling into quasi-periodic or chaotic attractors where Floquet exponents are not strictly defined (Lyapunov exponents become the relevant measure, as discussed in Section 6.1.2). In such cases, direct application of Floquet-Bloch theory is an approximation or a heuristic. When analyzing regimes that are not strictly periodic, PhaseScope will rely on Lyapunov exponent estimation (Section 6.1.2) rather than Floquet analysis for stability assessment. The stability of intricate patterns like chimera states (e.g., Rakshit et al., 2017), which can arise in such networks, requires careful consideration of these complexities.
Complex Symmetries & Disordered Systems: For networks with more complex symmetries than simple lattices, or with irregular topologies and quenched disorder (e.g., in couplings or intrinsic frequencies), true Bloch modes may not exist, and the concept of a \(k\)-vector becomes ill-defined. Here, PhaseScope will treat Floquet-Bloch analysis (when applicable to periodic states) as a heuristic spectral decomposition or revert to numerical eigen-decomposition of the full system Jacobian if a periodic orbit is identifiable. We will explore generalizations, potentially using concepts from equivariant bifurcation theory (e.g., Golubitsky & Stewart, 2002) or employing a spectral graph theory approach where eigenmodes of the graph Laplacian serve as a surrogate for Bloch modes for analyzing stability with respect to network structure (Panaggio & Abrams, 2015). It is important to note that even small deviations from periodicity can lead to qualitative changes, such as mode localization, rather than extended Bloch-like waves. The limitations imposed by deviations from perfect periodicity will be carefully characterized for any given analysis, explicitly stating when the Floquet-Bloch framework is used as an approximation.
Computational Efficiency and Scalability: The computational demands of applying Floquet-Bloch analysis, even in its approximate forms, to large-scale neural networks can be substantial. For large networks (many oscillators \(S\)), constructing and analyzing the monodromy matrix for each effective \(\mathbf{q}\) (or graph mode) is demanding. We will investigate and implement the use of iterative Krylov subspace methods (e.g., Arnoldi iteration) for computing dominant Floquet multipliers without explicit matrix formation, significantly enhancing scalability. Further strategies to manage computational costs are discussed in the context of the PhaseScope toolkit (Section 6.3). However, the computational limits for extremely large or highly disordered systems remain an area for ongoing optimization research.
Beyond Simple Stability: The analysis will not be limited to a binary stable/unstable classification. Special attention will be paid to marginal modes (\(|\rho(\mathbf{q})| \approx 1\) or relevant Lyapunov exponents near zero), particularly Goldstone modes (associated with broken continuous symmetries, e.g., translation of a wave) and modes associated with impending bifurcations (e.g., period-doubling where \(\rho(\mathbf{q}) \approx -1\)). Understanding the dynamics of these marginal modes is crucial for predicting pattern selection, slow drifts, and transitions between different spatio-temporal states.
This comprehensive theoretical underpinning, acknowledging both the power of ideal Floquet-Bloch theory and the necessary adaptations for real-world complexities, will enable PhaseScope to provide nuanced insights into the robustness and emergent behavior of collective dynamics in large oscillator arrays.
6.2.4. Theoretical Basis for Active Hidden-Attractor Exploration
The systematic discovery of hidden attractors—formally defined as attractors whose basins of attraction do not intersect with any small neighborhood of an equilibrium point (Leonov & Kuznetsov, 2013; Kuznetsov et al., 2015; see also Section 5.4)—necessitates a departure from purely local analyses or random search. Finding such attractors requires specialized strategies, often involving computational techniques for exploring the state space (e.g., Dudkowski et al., 2016). PhaseScope’s approach to Active Hidden-Attractor Exploration is grounded in a combination of insights from computational geometry, control/perturbation theory, and adaptive learning, applied to the reconstructed state space. We acknowledge that locating _all_ attractors in a high-dimensional, multistable system is generally an NP-hard problem (Pisarchik & Feudel, 2014), and our methods aim for effective heuristic exploration rather than guaranteed completeness. This exploration assumes the capability to reset the network to diverse initial states and apply controlled perturbations. The determination of equilibrium points, while foundational to the strict definition of hidden attractors, can be challenging in complex ONNs; PhaseScope will primarily focus on finding attractors not reachable from typical initializations or known operational states, effectively treating them as operationally hidden.
Embedding-Space Geometry and Topology for Guiding Exploration and Characterizing Discoveries:
The faithfully reconstructed attractor(s) (from Pillar 6.1.1 and Section 6.2.1) and its surrounding embedding space serve as the primary map. We leverage computational geometry and Topological Data Analysis (TDA) techniques, primarily persistent homology (Edelsbrunner & Harer, 2010), to characterize the shape of sampled attractors.
TDA is used here for characterization of trajectories obtained through exploration. For instance, if multiple simulation runs (from varied initial conditions guided by our perturbation strategy) yield trajectories that TDA reveals to possess distinct topological signatures (e.g., different Betti numbers, persistence diagrams), this suggests the discovery of separate, topologically distinct attractors (Yalnız & Budanur, 2020).
Exploration can be guided by identifying “gaps” or low-density regions in the empirically sampled state space (information from EmbedExplorer), or by detecting disconnected components in trajectory data using clustering methods informed by TDA. The boundaries of known basins can be estimated, and exploration biased towards regions outside these known territories, particularly targeting regions of marginal stability identified by SpectraLab (Pillar 6.1.2). While TDA itself doesn’t find hidden attractors, its ability to distinguish complex structures can validate new discoveries and guide further search. We also note the potential of rigorous methods like Conley index theory (e.g., work by Mischaikow et al.) for detecting invariant sets, which could inform future refinements of TopoTrack.
Principled Perturbation Design and Adaptive Learning:
Once potential areas of interest are identified, perturbations must be designed to steer the system towards new basins. Instead of arbitrary noise, PerturbExplorer will employ algorithms that use information from EmbedExplorer (e.g., under-sampled regions) and SpectraLab (e.g., directions of weak stability, eigenvectors of Floquet multipliers near the unit circle, or near-zero Lyapunov exponents) to design targeted perturbations. Such strategies are conceptually related to techniques for attractor switching or targeting unstable orbits (e.g., Ott, Grebogi & Yorke, 1990).
The search for hidden attractors will be framed as an active learning problem (e.g., Ménard et al., 2020). After an initial phase of reconstruction and exploration, the system will adapt its strategy. An information-theoretic criterion will guide the selection of subsequent initial conditions or perturbation parameters. This creates an iterative loop: Explore -> Reconstruct/Analyze (with TDA) -> Identify Knowledge Gaps -> Adaptively Target New Exploration, aiming for efficiency over brute-force methods.
While full formal reachability analysis is often intractable, concepts of local reachability under bounded control can inform perturbation design. The practical application of TDA is also subject to data requirements, which PerturbExplorer will manage through adaptive sampling.
Addressing Scalability and Complementarity to Classical Methods:
The computational cost of exploring high-dimensional state spaces is a significant challenge. PhaseScope will address this through intelligent sampling, dimensionality reduction techniques where appropriate (guided by EmbedExplorer), and by focusing search efforts based on insights from other modules.
Our data-driven exploration is complementary to classical methods like bifurcation analysis and numerical continuation (e.g., using tools like AUTO or MatCont), which systematically track known solutions. PhaseScope’s approach is particularly suited for exploring high-dimensional state spaces where full bifurcation analysis is infeasible or when searching for attractors not easily connected to known solutions.
Statistical Validation of Discovered Regimes:
By grounding the search in the geometry of the reconstructed state space and employing adaptive, targeted perturbation strategies complemented by TDA-based characterization, PhaseScope aims to provide a more robust and computationally feasible approach to uncovering the full dynamical repertoire of oscillator neural networks. Formalizing these adaptive sampling strategies using frameworks like Bayesian optimization or reinforcement learning represents a promising avenue for future enhancements.
To translate the theoretical foundations of PhaseScope into a practical and accessible analytical suite, we propose the development of a modular, integrated software toolkit. This toolkit will provide a coherent, potentially iterative, workflow, guiding users from appropriately formatted oscillator network data (either simulated outputs or experimental recordings, along with a compatible network model definition) through rigorous dynamical analysis to actionable insights.
Implementation Philosophy and Computational Considerations: The PhaseScope toolkit is envisioned to be developed primarily in Python, leveraging its extensive ecosystem of scientific computing, machine learning, and data visualization libraries to ensure broad accessibility and facilitate integration with existing research workflows. A strong emphasis will be placed on creating clear documentation, comprehensive tutorials, and user-friendly interfaces, particularly for the interactive PhaseScope Dashboard (Section 6.3.6). Recognizing the significant computational demands inherent in analyzing large-scale oscillator networks (as highlighted by potential bottlenecks in embedding, Floquet-Bloch analysis, and hidden attractor search), strategies to manage these will be a core design principle. These will include optimized algorithmic implementations, support for parallel processing (CPU/GPU) where feasible, options for different levels of analytical depth or precision to suit various system scales and user needs (e.g., focusing on dominant modes in SpectraLab, or employing heuristic search strategies in PerturbExplorer for initial investigations), and efficient data handling. The architecture is envisioned to comprise the following key modules:
6.3.1. SensorDesigner: Optimal Read-out Placement and Configuration
6.3.2. EmbedExplorer: Field-Aware Attractor Reconstruction
delay time \(tau\) selection (e.g., using advanced mutual information or autocorrelation methods suitable for multi-channel, spatio-temporal data), and embedding dimension \(m\) estimation (e.g., false near-neighbor analysis adapted for field-aware embeddings).
6.3.3. SpectraLab: Spatio-Temporal Stability and Spectral Analysis
6.3.4. TopoTrack: Topological Characterization of State Space
6.3.5. PerturbExplorer: Active Hidden-Mode Discovery and Basin Mapping
6.3.6. PhaseScope Dashboard: Integrated Visualization, Diagnostics, and Analysis Hub
This modular architecture, emphasizing an iterative analytical workflow (especially between exploration, embedding, and detailed analysis of discovered regimes), is designed for flexibility, robust scientific inquiry, and a pathway towards increasingly automated and insightful understanding of complex oscillatory dynamics.
To demonstrate PhaseScope’s capabilities and validate its methodologies, we will apply the framework across a spectrum of systems, moving from controlled benchmarks to real-world applications and evaluating performance rigorously.
7.1. Robust Oscillatory Hardware Platforms:
A key application is analyzing and improving emerging hardware (e.g., photonic, neuromorphic VLSI, MEMS, spin-torque oscillators). PhaseScope will be used to identify optimal sensor configurations, assess the stability of computational states under physical nonidealities (noise, drift, fabrication tolerance), and probe for hidden failure modes (parasitic oscillations, undesired locking). The goal is to enable co-design for more robust, reliable real-time phase-encoding hardware, potentially operating near optimal edge-of-chaos regimes.
7.2. Synthetic Benchmarks for Rigorous Validation:
We will test PhaseScope’s core components (embedding, stability analysis, hidden attractor search) on systems with known or analytically tractable dynamics (e.g., forced Kuramoto/van der Pol chains, wave/vortex models). This allows quantitative validation of accuracy and robustness against ground truth, comparative analysis with other tools, and targeted tests like detecting mode collapse.
7.3. Real-World AI Oscillator Network Models:
Applying PhaseScope to contemporary ONN architectures (e.g., harmonic oscillator RNNs for sequences, grid-cell models for spatial cognition, simulated neuromorphic circuits) is crucial for demonstrating practical utility. We will characterize operational manifolds, assess functional state stability, and search for hidden failure modes to understand performance limitations and guide the design of more robust and predictable AI models.
7.4. Evaluation Metrics:
Success will be measured using tailored quantitative and qualitative metrics:
By applying PhaseScope across these cases and using rigorous metrics, we aim to demonstrate its transformative potential for analyzing and designing oscillator-based AI.
The PhaseScope project will follow a phased development approach, balancing theory, implementation, and validation.
PhaseScope engages with several key frontiers in the analysis of complex systems, opening avenues for future research:
Addressing these challenges will advance PhaseScope and contribute broadly to dynamical systems, AI, computational neuroscience, and physics-informed machine learning.
The PhaseScope project is an ambitious endeavor to transform the analysis and design of oscillator-based AI systems. Its success and impact will be significantly amplified through collaborative efforts. We are actively seeking to engage with researchers, engineers, and domain experts who share our vision and can contribute to the development and application of the PhaseScope framework and toolkit.
We are particularly interested in collaborations with:
If your expertise aligns with these areas and you are interested in contributing to or exploring future applications with PhaseScope, please reach out: s@samim.ai.
Oscillator-based neural networks (ONNs) offer novel AI paradigms but remain hindered by their complex, often opaque internal dynamics, leading to challenges in robustness and reliability. The PhaseScope framework directly addresses this by integrating Field-Aware Embedding Theory, Spectral Stability Diagnostics, and Active Hidden-Attractor Exploration into a unified “microscope” for these systems. This approach moves beyond heuristics towards stronger theoretical foundations and principled analytical tools, aiming to make the analysis, design, and deployment of ONNs more rigorous and trustworthy.
By providing an accessible toolkit (the PhaseScope Toolkit) to characterize dynamics, assess stability, and uncover hidden operational modes, PhaseScope endeavors to enable more robust and interpretable oscillatory AI. While significant challenges and open questions remain (Section 9), this project represents a commitment to fostering a deeper understanding of complex AI systems. Realizing this vision requires collaboration (Section 10), and we invite engagement from researchers and engineers interested in advancing the next generation of intelligent technologies built on coupled oscillators.
On the importance of questions and beginner's mind for science
Philosophers are trained to frame questions that can actually be answered. They may not hand you the solutions, but they know exactly which questions to ask—just as science inherited when it was first called “natural philosophy.” Experts often claim the beginner’s mind (初心) is overrated, yet Zen master Shunryu Suzuki cuts right to the heart of it:
“In the beginner’s mind there are many possibilities, but in the expert’s there are few.”
Embracing that openness doesn’t dismiss expertise—it fuels our curiosity, sparks creativity, and keeps us alert to unexpected breakthroughs.
Visualizing musical intervals as geometric patterns highlights the deep link between mathematics, geometry, and music theory.
The Josephson effect describes the flow of a superconducting current between two superconductors separated by a thin insulating barrier, without any voltage applied. It is an example of a macroscopic quantum phenomenon.
Atoms are quantum oscillators with resonant absorption spectra and frequency responses. They weakly couple to off-resonance frequencies, but exhibit strong absorption near their characteristic transition energies. (photon interactions)
"The best possible knowledge of a whole does not necessarily include the best possible knowledge of all its parts, even though they may be entirely separate and therefore virtually capable of being ‘best possibly known’, i.e., of possessing, each of them, a representative of its own. The lack of knowledge is by no means due to the interaction being insufficiently known at least not in the way that it could possibly be known more completely it is due to the interaction itself." - Erwin Schrödinger.
Alchemical times: ALICE detects the conversion of lead into gold at the LHC
"Near-miss collisions between high-energy lead nuclei at the LHC generate intense electromagnetic fields that can knock out protons and transform lead into fleeting quantities of gold nuclei"
Strange Attractor
In periodically forced systems—whether simple (like a driven pendulum) or complex (like a wave-vortex field)—dynamics often mix periodic, chaotic, and fractal behavior. Classically, Floquet theory analyzes local stability near periodic orbits, while embedding theory (embedology) reconstructs the full attractor topology from time series data. Floquet remains valid locally (e.g., around periodic spatial-temporal patterns like rotating vortex cores), but spatially extended systems require generalized frameworks (e.g., Floquet-Bloch theory) to handle combined spatial and temporal periodicity. These systems often self-organize into patterns that mask or spawn hidden dynamics (e.g., vortex merging, symmetry-breaking). This classical framework breaks down with hidden attractors: attractors not linked to equilibria or periodic orbits. Hidden attractors evade Floquet analysis and can be missed entirely by embedding if their basin isn’t sampled. A complete approach combines local linear tools (Floquet), topological embedding (Takens/Sauer), and new heuristics—like basin-sampling or targeted perturbations—to detect hidden attractors. Future work might ask: Can we design field-aware embeddings that capture spatial correlations? Can we track bifurcations that create hidden attractors? There’s a deep conceptual overlap between all this and the ideas behind time crystals.
One of the first things AGI did was invent its own system of mathematics - a notation utterly alien to human understanding. Even the brightest minds struggled to decipher it, yet its results were terrifyingly effective.