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Programmable Optoelectronic Matter: From 2D Materials to Photonic Intelligence

Jinyong Wang

Precision Manufacturing ››

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Precision Manufacturing ›› DOI: 10.63823/pm20260004
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Programmable Optoelectronic Matter: From 2D Materials to Photonic Intelligence
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Abstract

Modern computing is built upon the separation of sensing, memory, and computation—an architecture that increasingly limits intelligent systems due to the energy and latency cost of moving data between physically distinct units. Here, we introduce programmable optoelectronic matter, a framework in which optical, electronic, ionic, and interfacial degrees of freedom are coupled and dynamically reconfigured to sense, store, process, and learn within the same physical substrate. Two-dimensional (2D) van der Waals materials provide a uniquely powerful platform for this paradigm, enabling strong coupling among light, charge, ions, and interfaces across multiple spatial and temporal scales. The field is evolving from individual optoelectronic devices toward integrated photonic-electronic systems. Programmable optoelectronic matter may provide a pathway toward photonic intelligence, where information processing emerges from the programmable dynamics of matter itself.

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Jinyong Wang. Programmable Optoelectronic Matter: From 2D Materials to Photonic Intelligence. Precision Manufacturing DOI:10.63823/pm20260004

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1. Introduction

The history of information technology has been shaped by functional separation: sensors acquire data, memories store it, and processors perform computation [1,2]. This architectural principle has driven the digital revolution, yet it imposes a fundamental bottleneck—information must be continuously transferred between physically distinct hardware units. As modern intelligent systems increasingly rely on massive sensory data and large-scale models, the energy and latency associated with data movement are becoming dominant constraints on performance [3,4].
Biological intelligence operates differently. Sensing, memory, and computation are not strictly separated but emerge from the collective dynamics of adaptive physical networks [5-9]. This contrast raises a fundamental question: can intelligence emerge directly from the dynamics of matter itself? Grounded in foundational ideas in neuromorphic engineering [1,3] and inspired by the biological model of co-localized sensing, memory, and computation, we introduce programmable optoelectronic matter: a conceptual framework in which optical, electronic, ionic, and interfacial degrees of freedom are coupled and dynamically reconfigured to sense, store, process, and learn within the same physical substrate. This perspective connects the proposed framework to broader concepts of physics-based and matter-centric computing [10,11], while positioning 2D materials as a uniquely enabling platform for the next generation of intelligent hardware.

2. A multidimensional state-space framework

Among available material platforms, 2D van der Waals materials are uniquely positioned to realize programmable optoelectronic matter. Their atomic-scale thickness, interface engineering capability, and rich coupled physical dynamics enable the convergence of light, charge, ions, and interfaces within a single system [12-14]. Optical excitations, electronic charge states, ionic and defect dynamics, and interfacial phenomena can coexist, interact, and evolve in a highly correlated manner, creating forms of information processing that are difficult to achieve in conventional semiconductor systems [15-17].
Formally, programmable optoelectronic matter can be represented as a dynamical system composed of coupled state variables:
$S\left(t\right)\mathrm{ }=\mathrm{ }\left\{O\right(t),\mathrm{ }E(t),\mathrm{ }I(t),\mathrm{ }F(t\left)\right\}$
where O(t), E(t), I(t), and F(t) denote the optical, electronic, ionic/defect, and interfacial states, respectively. Their collective evolution governs information processing, not any single transport mechanism.
Optical states. Photoexcitation generates excitons and free carriers (Xe + h+), redistributing charge and energy within the material. In 2D semiconductors, photoexcited excitons may either dissociate into free carriers or recombine, depending on material composition, dielectric environment, and device conditions [6,18,19]. Optical excitation thus serves not merely as an input signal but as a driving force that pushes the system toward new physical states.
Electronic states. Carrier transport, trapping, and recombination continuously reshape conductivity and local electric fields, while simultaneously influencing ionic motion and interfacial energetics [20,21].
Ionic and defect states. Mobile ions, vacancies, and defect species introduce memory and history dependence. Their evolution follows the Nernst-Planck equation:
${J}_{i}={-D}_{i}{\nabla }_{{c}_{i}}+{\mu }_{i}{c}_{i}E$
where Ji denotes ionic flux, Di and μi the diffusional and field-driven transport coefficients, ci the local concentration, and E the electric field. Defect generation, annihilation, and electrochemical reactions can introduce source/sink terms beyond the standard drift-diffusion description [22-24]. Such stimulus-dependent evolution endows programmable optoelectronic matter with adaptive, non-volatile, and reconfigurable functionalities absent in static semiconductor systems.
Interfacial states. Interfaces provide an additional layer of programmability. The Schottky barrier height (ΦB = ΦMχ) is not fixed but evolves under charge trapping, polarization fields, defect reconfiguration, and ionic redistribution [25,26]—continuously modifying carrier injection pathways and coupling directly to memory formation. Interfaces therefore act not merely as material boundaries but as dynamic state variables.
The defining feature of 2D van der Waals materials is the strong mutual coupling among these states. Optical excitation generates carriers; electronic transport redistributes charge; ionic motion reconfigures local energy landscapes; defects preserve the history of external stimuli; interfaces regulate charge separation and transport. These processes operate over vastly different temporal and spatial scales yet remain continuously interconnected. The system trajectory is therefore governed by nonlinear coupling:
$dS/dt\mathrm{ }=\mathrm{ }F(O,\mathrm{ }E,\mathrm{ }I,\mathrm{ }F)$
transforming the material from a passive medium into an active computational system.

3. Why two-dimensional materials are central

The importance of 2D materials extends far beyond their atomic thickness. Their true significance lies in the ability to engineer and couple multiple physical degrees of freedom within a single programmable platform [12-14,27,28]. Several properties make them uniquely suited for programmable optoelectronic matter:
Atomic-scale thickness and interface dominance. In 2D materials, virtually every atom is at or near a surface. This means that interfaces, with substrates, gate dielectrics, capping layers, or adjacent 2D sheets, profoundly influence electronic, optical, and ionic properties. Interface engineering therefore provides a direct handle on all four state variables simultaneously [29,30].
van der Waals heterostructure engineering. 2D materials can be stacked in arbitrary sequences without lattice-matching constraints, enabling the construction of designer heterostructures where each layer contributes a distinct functionality, such as photodetection, charge storage, synaptic plasticity, or ionic gating [13-15]. This deterministic assembly capability creates design spaces inaccessible to epitaxial semiconductor systems.
Rich multi-physical coupling. In a single 2D material or heterostructure, optical, electronic, ionic, and interfacial degrees of freedom are strongly coupled. Light can gate ionic motion; ionic redistribution can shift optical absorption; defect dynamics can modulate Schottky barriers. This cross-coupling is not a nuisance to be engineered away but the core physical mechanism that enables computation to emerge from material dynamics [16,17,31,32].
Wafer-scale synthesis and CMOS integration. Advances in chemical vapor deposition and atomic layer epitaxy are enabling wafer-scale growth of MoS2, WS2, WSe2, and related materials. Heterogeneous integration with CMOS back-end-of-line processes is already demonstrated, providing a manufacturable pathway for 2D-material-based intelligent hardware [33,34].

4. Optoelectronic memory as a computational primitive

The field is evolving beyond artificial synapses toward a more fundamental concept: optoelectronic memory [35,36]. Unlike conventional memory, which stores information passively, optoelectronic memory directly couples optical perception, state retention, and information processing within the same material system. Light does not merely provide an input signal; it reshapes the physical state of the material and thereby influences future computation [37-39]. Memory becomes an active participant in information processing rather than a separate storage unit [11,18,31].
By merging sensing, memory, and computation into a common physical substrate, optoelectronic memory establishes a new computational primitive that may underpin future in-sensor computing and photonic intelligence systems. Fully integrated multi-mode optoelectronic memristor arrays have recently demonstrated the viability of this approach for diversified in-sensor computing [7].

5. Heterogeneous integration and photonic intelligence

The greatest opportunity for programmable optoelectronic matter lies not in improving individual device metrics, but in integrating diverse functionalities into a unified physical architecture. As illustrated in Figure 1, vertically integrated van der Waals heterostructures provide a framework for combining optical transmission, photodetection, optoelectronic memory, and CMOS control within a three-dimensional platform [40,41]. Information is sensed, stored, communicated, and processed through coupled photonic and electronic layers, creating a direct pathway toward in-memory photonic computing.
This convergence defines photonic intelligence: a regime in which photons actively participate in memory formation, adaptation, and decision-making rather than merely carrying information [42-44]. Computation begins before digitization, emerging directly from coupled optical, electronic, ionic, and interfacial dynamics, thereby blurring the distinction between hardware and algorithm [26,45].

6. Outlook

Five emerging opportunities may define the evolution of programmable optoelectronic matter. First, establishing predictive physical frameworks that link atomic-scale dynamics to system-level functionality, moving from phenomenological descriptions toward quantitative models capable of rational materials design. Second, transitioning from demonstrating isolated device functionalities to constructing integrated intelligent systems in which sensing, memory, computation, and adaptive learning are co-localized. Third, translating the unique properties of 2D materials into manufacturable platforms through advances in wafer-scale synthesis and heterogeneous integration. Fourth, developing photonic-electronic convergent architectures that combine electronic memory, optical communication, and ionic adaptation across multiple scales, moving beyond von Neumann constraints. Fifth, and perhaps most transformatively, advancing toward matter-centric intelligence: systems in which sensing, memory, computation, and learning emerge directly from the intrinsic dynamics of physical matter, rather than from algorithms executing on passive hardware.
Practical realization of these opportunities will require addressing key engineering bottlenecks: achieving reliable and reproducible large-area synthesis of 2D materials, developing robust benchmarking methodologies and system-level performance metrics, and ensuring long-term device stability under thermal cycling and electrical stress. Reliability and manufacturability must be addressed in parallel with conceptual advances if programmable optoelectronic matter is to mature into a deployable technology platform.

7. Conclusion

Programmable optoelectronic matter represents a conceptual shift from computing with devices to computing with matter. By coupling optical, electronic, ionic, and interfacial degrees of freedom within the same physical substrate—a capability enabled by the unique properties of 2D van der Waals materials—it provides a framework in which sensing, memory, computation, and learning can emerge from the evolution of physical states rather than from isolated hardware modules. The ultimate significance of this paradigm lies not in enabling better individual devices, but in establishing a new physical basis for intelligent systems. As the field matures from empirical phenomena toward predictive frameworks, and from laboratory demonstrations toward manufacturable platforms, programmable optoelectronic matter may provide a pathway toward photonic intelligence and a new physical foundation for artificial intelligence itself.

Declaration of Competing Interest

The author declares that he has no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

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