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  <id>https://arxiv.org/api/3bncLZ6lIr75yyG6jwi4dEWBeVs</id>
  <title>arXiv Query: search_query=all:"quantum programming language" OR all:"photonic computing" OR all:"programming language" AND cat:quant-ph&amp;id_list=&amp;start=0&amp;max_results=60</title>
  <updated>2026-09-26T15:46:56Z</updated>
  <link href="https://arxiv.org/api/query?search_query=all:%22quantum+programming+language%22+OR+(all:%22photonic+computing%22+OR+(all:%22programming+language%22+AND+cat:quant-ph))&amp;start=0&amp;max_results=60&amp;id_list=" type="application/atom+xml"/>
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  <entry>
    <id>http://arxiv.org/abs/2609.22015v2</id>
    <title>Optical Mode Sorting with a Programmable Diffractive Neural Network</title>
    <updated>2026-09-22T08:09:23Z</updated>
    <link href="https://arxiv.org/abs/2609.22015v2" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2609.22015v2" rel="related" type="application/pdf" title="pdf"/>
    <summary>Programmable diffractive optical processors are particularly attractive for spatial light manipulation because their optical transformations can be dynamically reconfigured and adapted without modifying the physical hardware. However, their practical performance is often limited by the gap between simulation and experiment caused by optical aberrations, alignment errors, and nonideal phase responses. In this paper, we introduce a hybrid optimization framework that combines high-dimensional numerical design with low-dimensional hardware-in-the-loop calibration, enabling programmable diffractive optical networks to compensate experimentally for mismatch without retraining their underlying optical transformations. We demonstrate a programmable optical diffractive neural network (ODNN) designed by back-propagation to spatially sort six linearly polarized modes supported by a multimode fiber. The experimental distortions are represented using a truncated Zernike basis with only 19 correction coefficients per layer. These coefficients are optimized directly on the physical system using stochastic parallel gradient descent, avoiding re-optimization of the full pixelated phase masks. Experimentally, the proposed calibration yields an SNR improvement of approximately 3.26 dB, and a decrease in amplitude error of 0.04. This separation of high-dimensional optical-function design from low-dimensional physical calibration provides a scalable route towards adaptive and reconfigurable spatial-mode processors for optical router on spatial modes and wavelengths, programmable photonic computer systems and quantum information processing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-09-18T17:10:40Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Qian Zhang</name>
    </author>
    <author>
      <name>Shiyue Chen</name>
    </author>
    <author>
      <name>Juergen W Czarske</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2609.06796v1</id>
    <title>Hardware Trojan Threats to Multi-Chiplet Photonic Neural Network Accelerators</title>
    <updated>2026-09-06T19:35:19Z</updated>
    <link href="https://arxiv.org/abs/2609.06796v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2609.06796v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Multi-chiplet photonic neural network accelerators (MCPNAs) combine photonic computation, photonic communica-tion, and heterogeneous chiplet integration to enable scalable and energy-efficient AI acceleration. However, their distributed archi-tecture and reliance on third-party chiplets introduce significant hardware security risks. This paper examines Hardware Trojan (HT) threats to MCPNAs across three dimensions: confidentiality, integrity, and availability.</summary>
    <category term="cs.AR" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.AI" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.LG" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-09-06T19:35:19Z</published>
    <arxiv:primary_category term="cs.AR"/>
    <author>
      <name>Sudeep Pasricha</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2609.03802v1</id>
    <title>Quantum Query Complexity of Finding a Tarski Fixed Point on a High-Dimensional Grid</title>
    <updated>2026-09-03T13:06:12Z</updated>
    <link href="https://arxiv.org/abs/2609.03802v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2609.03802v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>The Knaster-Tarski fixed-point theorem states that every monotone function over a complete lattice has a fixed point. Beyond its fundamental role in order theory, the theorem and its algorithmic variants have found broad applications in areas such as economics, game theory, and programming languages. While the query complexity of finding a Tarski fixed point has been extensively studied in classical models, comparatively little is known in the quantum setting.
  We prove an $Ω(k\log n)$ quantum query lower bound for finding a fixed point of a monotone function on $[n]^k$, using the nonnegative spectral adversary method. In the two extremal regimes $n = 2$ and $k = 1$, our quantum lower bound matches the previous classical lower bounds $Ω(k)$ and $Ω(\log n)$, respectively. For $n, k\geq 2$, our bound improves the best previous classical lower bound when $n &lt; k$ and is within a factor of $\log n / \log k$ compared to the known classical lower bound when $n \geq k$. To construct the adversary matrix, we develop the Tree--Filtration Adversary Method. Besides yielding our lower bound, the method offers a more transparent combinatorial interpretation of the nonnegative spectral adversary method. When the hard instances of a problem admit a tree-like organization and suggest an intuition analogous to classical decision-tree lower bounds, our method provide a promising approach to establishing quantum complexity lower bounds.</summary>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.CC" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.DS" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-09-03T13:06:12Z</published>
    <arxiv:comment>35 pages, 5 figures</arxiv:comment>
    <arxiv:primary_category term="quant-ph"/>
    <author>
      <name>Tongyang Li</name>
    </author>
    <author>
      <name>Weiran Ma</name>
    </author>
    <author>
      <name>Ziyi Yang</name>
    </author>
    <author>
      <name>Xingyu Zhao</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2608.28048v1</id>
    <title>AI Hardware Accelerators for Large Language Models: Architectures and the Memory Wall</title>
    <updated>2026-08-28T08:10:01Z</updated>
    <link href="https://arxiv.org/abs/2608.28048v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2608.28048v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Large language models (LLMs) place unprecedented and still-growing demands on the hardware that trains and serves them. This review surveys the full landscape of AI hardware accelerators for LLMs, including general-purpose GPUs, custom ASICs such as TPUs, Trainium, Groq, and Cerebras, reconfigurable FPGAs, processing-in-memory and near-memory architectures, and emerging neuromorphic and photonic approaches across cloud and edge deployment. Using the transformer's computational structure and roofline analysis as a common framework, we show that the decisive constraint on LLM acceleration is not arithmetic but memory: the autoregressive decode phase is bandwidth-bound, the key-value cache can rival the model weights in size, and data movement dominates energy. Comparing platforms on compute, memory, energy, programmability, and scalability, we find that no single architecture is optimal across workloads: GPUs remain the flexible default and the workhorse of training; domain-specific ASICs win at scale for stable, high-volume workloads; processing-in-memory is the most promising near-term response to the memory wall, entering systems as a heterogeneous complement; and neuromorphic and photonic computing, while promising, are not yet production-ready at frontier scale. Future progress depends on hardware-algorithm co-design and heterogeneous, memory-centric systems: for large language models, the memory system has become the computer.</summary>
    <category term="cs.AR" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.DC" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-08-28T08:10:01Z</published>
    <arxiv:comment>Review/survey article on AI hardware accelerators for large language models; compares GPUs, ASICs, FPGAs, processing-in-memory/near-memory, neuromorphic, and photonic architectures</arxiv:comment>
    <arxiv:primary_category term="cs.AR"/>
    <author>
      <name>Siddharth Patel</name>
    </author>
    <author>
      <name>Rohit Singh</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2608.20443v3</id>
    <title>Granthi: Higher-Order Quantum Programming via Unitary Wiring</title>
    <updated>2026-09-08T14:51:19Z</updated>
    <link href="https://arxiv.org/abs/2608.20443v3" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2608.20443v3" rel="related" type="application/pdf" title="pdf"/>
    <summary>Many mainstream quantum programming languages confine higher-order structure to a classical host while restricting the quantum layer to first-order operations on qubits. This paper presents Granthi, a purely unitary higher-order quantum programming language built on three design commitments: quantum programs are first-class values that may be passed, returned, and coherently composed; additive structure is tag-preserving routing rather than observational branching, so control may remain in superposition; and programmer-facing finite label types with staged reversible-operation bindings provide domain-level control spaces without exposing tag management. These bindings are eliminated by elaboration before Source typing.
  Granthi deterministically normalizes each Source program to a canonical wiring form. Every well-typed Source program, including a term of function type, has a unitary boundary interpretation. Under backend correctness (BC), the reference compiler produces a unitary circuit realizing that interpretation.
  Granthi's currently supported executable fragment is implemented end-to-end: an OCaml DSL elaborates surface programs through a higher-order Core IR to executable quantum circuits via pytket. The language directly supports the pure-unitary quantum switch for explicitly supplied operations; closed instances compile to static circuits. It also supports interference on control-flow history and structured finite control, all within the purely unitary fragment</summary>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.ET" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.LO" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.PL" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-08-20T15:49:09Z</published>
    <arxiv:comment>OOPSLA 2026. v3. New version with a corrigendum (fixing a soundness error in the typing of sums), and revised proofs of an expanded formal treatment of the compiler (v 1.0.2). Implementation: https://github.com/radhajagadeesan/granthi</arxiv:comment>
    <arxiv:primary_category term="quant-ph"/>
    <author>
      <name>Samson Abramsky</name>
    </author>
    <author>
      <name>Radha Jagadeesan</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2608.16597v1</id>
    <title>Engineering Polarization Switching in VCSELs with Custom Aperture Shapes</title>
    <updated>2026-08-17T13:53:24Z</updated>
    <link href="https://arxiv.org/abs/2608.16597v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2608.16597v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>We experimentally fabricate and measure vertical-cavity surface-emitting lasers (VCSELs) with custom aperture shapes, demonstrating predictable polarization control and switching, supporting their use in photonic computation schemes like Ising machines with polarization-based information encoding.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-08-17T13:53:24Z</published>
    <arxiv:comment>4 pages, 2 figures. Presented at CLEO 2025</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <arxiv:journal_ref>CLEO: Applications and Technology 2025, Technical Digest Series (Optica Publishing Group, 2025), paper JPS200_47</arxiv:journal_ref>
    <author>
      <name>Zifeng Yuan</name>
    </author>
    <author>
      <name>Dewen Zhang</name>
    </author>
    <author>
      <name>Hong-Lin Lin</name>
    </author>
    <author>
      <name>Aaron Danner</name>
    </author>
    <arxiv:doi>10.1364/CLEO_AT.2025.JPS200_47</arxiv:doi>
    <link rel="related" href="https://doi.org/10.1364/CLEO_AT.2025.JPS200_47" title="doi"/>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2608.09578v1</id>
    <title>Quantum Uncomputation of Clean and Dirty Ancilla Qubits</title>
    <updated>2026-08-10T13:13:54Z</updated>
    <link href="https://arxiv.org/abs/2608.09578v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2608.09578v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Automatic uncomputation aims to provide programming-language-level support to facilitate the correct and safe use of ancilla qubits in quantum computing, but efforts have only been made for clean ancillas, leaving dirty ancillas unexplored. We present a unified formalization of the uncomputation of both clean and dirty ancillas. For the first time, we prove that checking the existence of uncomputation is coNP-hard. We introduce two complementary synthesis-oriented existence-checking methods: a rewrite-based normalization algorithm (RwUn) and a template-based reasoning system (TpUn) that guarantees uncomputation through structured Store-Use patterns. We implement prototypes of both methods in Qiskit and Python. Compared to the state-of-the-art Reqomp~\cite{reqomp}, RwUn achieves 100% coverage on practical complex-dependency benchmarks, twice the coverage on random classical circuits, and about 50% coverage on random quantum circuits beyond the scope of existing methods, demonstrating broader applicability.</summary>
    <category term="cs.PL" scheme="http://arxiv.org/schemas/atom"/>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-08-10T13:13:54Z</published>
    <arxiv:primary_category term="cs.PL"/>
    <author>
      <name>Chenke Liu</name>
    </author>
    <author>
      <name>Li Zhou</name>
    </author>
    <author>
      <name>Boning Meng</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2608.04573v1</id>
    <title>Resource Estimation for Fault-Tolerant Quantum Programs</title>
    <updated>2026-08-05T08:02:46Z</updated>
    <link href="https://arxiv.org/abs/2608.04573v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2608.04573v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Fault-tolerant quantum computation enables the deployment of practical quantum algorithms but incurs substantial overhead from error correction, making resource estimation a central concern. Beyond case-by-case analyses, existing quantum programming languages either require programmers to manipulate low-level hardware details, rendering fault-tolerant implementations cumbersome, or abstract away the underlying error-correction schemes, reducing the effectiveness of resource utilization and estimation.
  To address these limitations while preserving programmability, we present a quantum programming language that enables efficient resource utilization, together with a resource-estimation framework for comprehensive resource analysis. Our framework features programmer-visible abstractions of error-correction schemes and cross-layer program-hardware analysis, allowing systematic exploration of resource trade-offs. We evaluate our approach on detailed fault-tolerant implementations of practical large-scale quantum algorithms, including components typically treated as black boxes in existing frameworks. The results demonstrate that our framework enables substantial resource savings while delivering detailed, fine-grained, and accurate resource estimates for fault-tolerant quantum programs.</summary>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.PL" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-08-05T08:02:46Z</published>
    <arxiv:primary_category term="quant-ph"/>
    <author>
      <name>Bonan Su</name>
    </author>
    <author>
      <name>Yuan Feng</name>
    </author>
    <author>
      <name>Li Zhou</name>
    </author>
    <author>
      <name>Mingsheng Ying</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.29543v1</id>
    <title>PROPEL: A Memory-Driven, Adaptive Vector-Flow-Field Router with Process-Aware Waveguide Generation for Large-Scale Photonic Integrated Circuits</title>
    <updated>2026-07-31T15:38:16Z</updated>
    <link href="https://arxiv.org/abs/2607.29543v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.29543v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Photonic integrated circuits (PICs) are increasing in scale and routing complexity, driven by photonic computing, optical switching, programmable interferometer meshes, wavelength-routed optical networks-on-chip, and chip-to-chip optical interconnects. Manual waveguide planning becomes impractical as designs approach thousands of photonic components because routing must satisfy geometric, optical, electrical, and manufacturing constraints. This paper presents the Photonic Routing Optimization and Placement Engine (PROPEL), a memory-driven, native-accelerated adaptive vector-flow-field routing framework with process-aware waveguide generation for large-scale PIC design. PROPEL builds a routing kernel based on a bounded vector-flow-field algorithm and DRC validation. The same kernel supports passive optical routing, active optical-electrical routing, and topology-driven net assignment. C++ accelerates field and routing calculations, while Python performs detailed DRC replay, legality checking, route commitment, and GDSFactory-based geometry generation. Compared with state-of-the-art routing solutions, PROPEL is faster on 17 of 18 shared passive-routing cases, with a median speedup of 2.6x and a geometric-mean speedup of 2.5x, while maintaining zero design-rule violations. PROPEL also supports length, delay, and optical-path-length matching, process-map-aware waveguide generation, route-memory reuse, selective rip-up/reroute, and GDS-level legality replay. These capabilities address heterogeneous PIC layouts where optical, electrical, process, topology, matching, and manufacturability constraints must be handled together.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-31T15:38:16Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>A Abdur Rahman Akib</name>
    </author>
    <author>
      <name>Eunso Shin</name>
    </author>
    <author>
      <name>Jonathan Rogers</name>
    </author>
    <author>
      <name>Jonathan Wierer</name>
    </author>
    <author>
      <name>Stanley Cheung</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.23137v1</id>
    <title>Reasoning about Continuous-Variable Quantum Systems</title>
    <updated>2026-07-25T10:36:34Z</updated>
    <link href="https://arxiv.org/abs/2607.23137v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.23137v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Continuous-variable quantum computing (CVQC) is a computing paradigm in which measurements yield values over a continuous domain. CVQC is both a convenient omputational framework for modeling physical quantum systems, and a good abstraction for hardware platforms based on quantum optics. Yet, the semantic foundations of CVQC remain underdeveloped. To address this gap, we develop a formal semantics for a core CV quantum programming language, and sound verification methods for program correctness.
  A main contribution of this work is to isolate a well-behaved quantitative predicate domain that achieves sufficient expressiveness to accommodate unbounded values as they arise in the infinite-dimensional, continuous setting. Specifically, we choose closed positive quadratic forms as semantic predicates, representing finite expectations, domains of finiteness, and infinite penalties in one ordered object. We validate our choice by establishing that our semantic predicates satisfy desirable closure properties including the definition of weakest preconditions.
  We validate our design with two case studies, including an example based on the celebrated GKP error-correcting code, for which we establish a second moment bound.</summary>
    <category term="cs.LO" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.PL" scheme="http://arxiv.org/schemas/atom"/>
    <category term="math.FA" scheme="http://arxiv.org/schemas/atom"/>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-25T10:36:34Z</published>
    <arxiv:comment>119 pages,2 figures</arxiv:comment>
    <arxiv:primary_category term="cs.LO"/>
    <author>
      <name>Tianshi Yu</name>
    </author>
    <author>
      <name>Gilles Barthe</name>
    </author>
    <author>
      <name>Minbo Gao</name>
    </author>
    <author>
      <name>Mingsheng Ying</name>
    </author>
    <author>
      <name>Li Zhou</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.20391v1</id>
    <title>Qoreo: Choreographic Programming for Quantum Distributed Systems</title>
    <updated>2026-07-22T17:25:15Z</updated>
    <link href="https://arxiv.org/abs/2607.20391v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.20391v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Programming distributed quantum systems requires multiple actors to coordinate precise sequences of quantum operations, classical communication, and entanglement generation. Writing such protocols directly as distributed processes is tedious and error-prone, and subtle mismatches can cause deadlock or silently incorrect quantum states. We present Qoreo, a choreographic programming language for quantum distributed systems in which an entire protocol is expressed as single, global program (a choreography) rather than as a collection of independent actor processes. Qoreo includes a local quantum language with linear types that enforce the no-cloning principle; a choreographic language that combines local quantum computation with inter-actor classical and quantum communication; and a process language for individual network nodes. We prove type safety for choreographies, guaranteeing that well-typed programs implement well-defined quantum operations, and we define endpoint projection~(EPP), which automatically derives a network of independent processes from any choreography. We prove EPP sound and complete with respect to the choreographic semantics; as a corollary, every well-typed choreography projects to a deadlock-free process network. The metatheory of Qoreo is fully mechanized in Rocq, and we provide an extraction pipeline to NetQASM for simulation and deployment on quantum network hardware.</summary>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.PL" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-22T17:25:15Z</published>
    <arxiv:primary_category term="quant-ph"/>
    <author>
      <name>Jennifer Paykin</name>
    </author>
    <author>
      <name>Steven Baldasty</name>
    </author>
    <author>
      <name>Joseph P. Near</name>
    </author>
    <author>
      <name>Christian Skalka</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.18061v1</id>
    <title>Programmable photonics enabled by ferroionic two-dimensional materials</title>
    <updated>2026-07-20T15:29:33Z</updated>
    <link href="https://arxiv.org/abs/2607.18061v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.18061v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Artificial intelligence (AI) models are scaling rapidly, exposing fundamental limitations in conventional computing architectures, where the physical separation of memory and computation imposes substantial energy and latency overheads. Optical neural networks offer a viable solution by enabling high-throughput, low-latency computation through the intrinsic parallelism of light. However, the scalability of photonic computing is constrained by the lack of materials that can provide low-loss, energy-efficient, and nonvolatile control of optical phase. Here, we discuss the emerging role of ferroionic two-dimensional materials as a platform for programmable photonics. Unlike conventional ferroelectrics, where polarization arises from bounded lattice distortions, ferroionic systems enable field-driven ionic redistribution, providing access to a continuum of stable and reconfigurable states. We outline how these material dynamics can be exploited to realize multi-level photonic states and nonvolatile phase control. Furthermore, we highlight a back-end integration strategy that introduces multifunctionality, including tunable optical nonlinearities into pre-fabricated photonic circuits without compromising optical performance. By bridging material-level dynamics with device- and system-level functionality, ferroionic materials provide a pathway toward reconfigurable, low-loss, and energy-efficient photonic computing architectures, opening new opportunities for neuromorphic and adaptive photonic systems.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-20T15:29:33Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Ghada Dushaq</name>
    </author>
    <author>
      <name>Srinivasa R Tamalampudiand</name>
    </author>
    <author>
      <name>Solomon Serunjogi</name>
    </author>
    <author>
      <name>Mahmoud Rasras</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.17817v1</id>
    <title>Photonic Memory as a Dynamical Phase for Neuromorphic Computing: A Unified Framework with Experimental Realization</title>
    <updated>2026-07-20T11:02:20Z</updated>
    <link href="https://arxiv.org/abs/2607.17817v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.17817v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Photonic memory underpins optical information processing, neuromorphic photonics, and photonic computing. Existing studies typically treat dispersive, nonlinear, and driven-dissipative memory as distinct physical phenomena, despite all being governed by the evolution of the optical field. This work proposes a unified phase-based framework in which photonic memory is interpreted as a dynamical phase, with transitions between memory regimes governed by optical phase evolution, Kerr nonlinearity, and the balance between delayed feedback and dissipation. Within this framework, dispersive memory arises from frequency-dependent phase accumulation, nonlinear memory emerges through intensity-dependent phase evolution leading to bistability and hysteresis, and driven-dissipative memory is established through attractor convergence and memory stabilization. The proposed framework is validated through theoretical analysis and numerical simulations, demonstrating a continuous progression from linear dispersive memory to nonlinear and ultimately driven-dissipative memory. Experimental validation is performed using a silicon photonic waveguide incorporating chirped Bragg gratings. Group delay measurements reveal distinct linear and nonlinear memory responses, while the reconstructed memory distribution demonstrates the coexistence of dispersive, nonlinear, and driven-dissipative memory within a single integrated photonic device. To the best of the author's knowledge, this constitutes the first experimental demonstration supporting the coexistence of all three photonic memory regimes in a single photonic platform. These results establish optical phase as the unifying physical quantity underlying photonic memory and provide a common framework for designing future neuromorphic photonic systems, reservoir computers, and integrated photonic processors.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-20T11:02:20Z</published>
    <arxiv:comment>9 pages, 10 figures</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Isaac Yorke</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.17714v1</id>
    <title>Formal Verification of Continuous-Variable Quantum Programs</title>
    <updated>2026-07-20T09:09:20Z</updated>
    <link href="https://arxiv.org/abs/2607.17714v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.17714v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>We provide a formal framework for Continuous-Variable Quantum Computing (CQC). While CQC is supported by photonic quantum hardware, we are not aware of a formal semantics for continuous-variable quantum programs nor of a unary Hoare logic for their verification. There are several technical obstacles to extending to CQC any of the formal frameworks available for Discrete-Variable Quantum Computing (DQC). Most importantly, continuous-variable quantum programs act on {\em infinite-dimensional} Hilbert spaces; their measurement outcomes are often {\em unbounded} and have expected values that are defined by an improper integral (or an infinite series), which may not converge. We overcome these challenges to give a formal semantics to a universal programming language for CQC and to provide the first Hoare logic for CQC. The assertions of our logic are built from polynomials over canonical observables. Besides proving relative completeness, we implement a symbolic weakest-precondition calculator for CQC based on our logic. Our tool has successfully verified CQC algorithms from textbooks and calculated their approximation errors for physically realizable implementations, proved the correctness (i.e., equivalence) of gate decompositions for CQC hardware, and computed the resource requirements (i.e., number of photon-number states) for achieving a desired accuracy in the classical simulation of continuous-variable quantum programs.</summary>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.LO" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-20T09:09:20Z</published>
    <arxiv:primary_category term="quant-ph"/>
    <author>
      <name>Stefanie Muroya</name>
    </author>
    <author>
      <name>Thomas A. Henzinger</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.16436v1</id>
    <title>Feynman Meets Turing: The Curse of Quantum Universality</title>
    <updated>2026-07-17T18:33:27Z</updated>
    <link href="https://arxiv.org/abs/2607.16436v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.16436v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>We consider a formal model of quantum circuit description languages (QCDLs) in which semantically meaningful programs correspond to computable unitary matrices. We show that any semantically universal QCDL -- that is, any QCDL able to describe all computable unitary matrices, which in turn form the set of matrices we can meaningfully represent on digital hardware -- cannot have a semi-decidable set of semantically meaningful descriptions. In particular, no such language admits a compiler that reliably recognizes all valid program descriptions. This result stands in contrast to classical programming languages. While compilation in languages such as C or C++ may itself involve non-terminating computations, the set of semantically meaningful programs remains recursively enumerable, since successful compilation provides a witness of validity. The essential difference lies in the nature of the semantic domains: classical languages describe partial recursive functions, whereas QCDLs describe total unitary operators. Our analysis establishes a fundamental limitation of quantum circuit description languages and highlights a structural distinction between classical and quantum models of computation at the level of formal language theory.</summary>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.FL" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-17T18:33:27Z</published>
    <arxiv:primary_category term="quant-ph"/>
    <author>
      <name>Yannik N. Böck</name>
    </author>
    <author>
      <name>Holger Boche</name>
    </author>
    <author>
      <name>Frank H. P. Fitzek</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.15873v1</id>
    <title>Programming with Quantum-Controlled Quantum Channels</title>
    <updated>2026-07-17T11:40:25Z</updated>
    <link href="https://arxiv.org/abs/2607.15873v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.15873v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>In contrast to a classical bit, which can only take the value $0$ or $1$, its quantum counterpart -- a qubit -- can exist in a superposition of $0$ and $1$. This is a superposition of data values, naturally raising the question of whether one can superpose not only data but also programs. For example, a particular superposition of programs, known as the quantum SWITCH, has attracted much attention, and its implementations and computational advantages have been studied extensively within the physics community.
  A naive way to control a program by a qubit is by means of a controlled operation. Given an operation $F$, this amounts to considering an operation that behaves as $F$ when the control qubit is $|1\rangle$, and as the identity operation when the control qubit is $|0\rangle$. This idea works well when $F$ is a unitary operation, but it is not well-defined for a general quantum channel. By contrast, the quantum SWITCH is free from the well-definedness issue. This contrast leads to the key insight of this paper: controlled operations and the quantum SWITCH should be regarded as different kinds of quantum control mechanisms.
  Building on this insight, we develop a novel quantum programming language with quantum control and measurement that can express the quantum SWITCH over quantum channels. Using a semantic analysis based on program transformations, we identify the source of the ill-behavedness of controlled operations as the \emph{correspondence problem}: a lack of coordination between the measurements performed in the then- and else-branches of quantum conditional branching. We address this problem with a linear type system that enforces alignment of the quantum operations used in the two branches, yielding a well-behaved language capable of expressing the quantum SWITCH.</summary>
    <category term="cs.PL" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.LO" scheme="http://arxiv.org/schemas/atom"/>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-17T11:40:25Z</published>
    <arxiv:comment>56 pages</arxiv:comment>
    <arxiv:primary_category term="cs.PL"/>
    <author>
      <name>Kengo Hirata</name>
    </author>
    <author>
      <name>Takeshi Tsukada</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.14477v1</id>
    <title>A generalized variational quantum linear solver on photonic platform</title>
    <updated>2026-07-16T01:49:19Z</updated>
    <link href="https://arxiv.org/abs/2607.14477v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.14477v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Based on a photonic computing platform, we experimentally validate a generalized variational quantum linear solver (VQLS) by systematically solving four-dimensional linear equation systems across different fields. In the complex field, in addition to solving non-singular systems that admit a unique solution, we investigate ill-conditioned problems arising from singularity--an issue frequently encountered in practical applications. To tackle these challenges, we introduce perturbation terms, a treatment inspired by Tikhonov regularization, and develop an algorithm capable of handling a wide range of systems. Furthermore, we extend the VQLS to the finite field F2 by redesigning the cost function to incorporate modulo 2 and imposing several constraints on the solution vector. This modulo 2 VQLS is inherently free from singularity. It is adapt to stabilizer coding theory and may find applications in areas such as decoders and the design of quantum gate sequences. Therefore, our work demonstrates the practical potential of VQLS in quantum computing, providing a solid experimental foundation and methodological guidance for its real-world applications.</summary>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-16T01:49:19Z</published>
    <arxiv:primary_category term="quant-ph"/>
    <author>
      <name>Kang Gao</name>
    </author>
    <author>
      <name>Zhao-An Wang</name>
    </author>
    <author>
      <name>Ze-Guo Wang</name>
    </author>
    <author>
      <name>Mao-Mao Huang</name>
    </author>
    <author>
      <name>Hai Wei</name>
    </author>
    <author>
      <name>Kai Wen</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.09605v1</id>
    <title>Quantum Orchestras: a Concrete Semantics for Recursive Hybrid Programs</title>
    <updated>2026-07-10T16:59:26Z</updated>
    <link href="https://arxiv.org/abs/2607.09605v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.09605v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Many production quantum programming languages represent hybrid quantum computations by extending a classical base language with a quantum effect, where qubits are addressed by reference, and quantum operations are understood to mutate some external quantum state. However, the semantics of this view of quantum computation remains underdeveloped, especially when the language allows mid-circuit measurements and non-termination.
  In this work, we provide a general method for building denotational semantics for such languages, by defining the quantum orchestra monad, which precisely captures this style of quantum effect. The monad has a concrete presentation, being based on the formalism of quantum instruments, a common tool in quantum information theory for capturing the action of a quantum process along with its classical outcomes. It acts on the category DCPO, and so enables the interpretation of divergent hybrid programs.
  The quantum orchestra monad serves as a natural extension of both the classical state monad and the probabilistic powerdomain monad. We investigate some of the subtleties present when trying to naïvely extend these definitions to the quantum non-commutative case.</summary>
    <category term="cs.PL" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.LO" scheme="http://arxiv.org/schemas/atom"/>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-10T16:59:26Z</published>
    <arxiv:comment>25 pages + 23 appendix</arxiv:comment>
    <arxiv:primary_category term="cs.PL"/>
    <author>
      <name>Alex Rice</name>
    </author>
    <author>
      <name>Dominik Leichtle</name>
    </author>
    <author>
      <name>Kim Worrall</name>
    </author>
    <author>
      <name>Robert I. Booth</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.09534v1</id>
    <title>Higher-Order Programs with Indefinite Causal Orders: a Linear Approach to Coherent Control of Quantum Processes</title>
    <updated>2026-07-10T15:38:33Z</updated>
    <link href="https://arxiv.org/abs/2607.09534v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.09534v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Processes with indefinite causal orders (ICOs), such as the quantum switch, are higher-order quantum processes that superpose the order in which quantum operations are performed. Such coherent control yields computational advantages but is not faithfully captured by existing quantum programming languages: either they are restricted to the unitary case, and thus cannot combine ICOs with measurement, or they treat coherent control nonlinearly. In both cases, they do not realize the full computational power of ICOs. We introduce a higher-order quantum functional language that supports general quantum computation, not merely the permutation of channels, and whose linear type system allows quantum control to be well-defined beyond the unitary case, on arbitrary quantum channels. We equip this language with a small-step operational semantics that synchronizes measurement outcomes across superposed branches, using device references and a memory function. We also give a denotational semantics by means of completely positive maps. With linearity as the only constraint, some well-typed terms would denote unphysical maps. We therefore impose a typing discipline that goes beyond linearity, and interpret programs in the causal category Caus[CPM], under which every well-typed program is physically meaningful, a property that can be checked statically and efficiently. We prove soundness, and study the language's expressive power: it can express every quantum channel at first order, and at second order a large subclass of the so-called quantum circuits with quantum control (QC-QCs), containing the quantum switch. Last but not least, we show that this language is well-designed enough to be extended to the nonlinear setting with recursion.</summary>
    <category term="cs.LO" scheme="http://arxiv.org/schemas/atom"/>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-10T15:38:33Z</published>
    <arxiv:primary_category term="cs.LO"/>
    <author>
      <name>Kathleen Barsse</name>
    </author>
    <author>
      <name>Romain Péchoux</name>
    </author>
    <author>
      <name>Simon Perdrix</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.08360v1</id>
    <title>Inverse-designed meta processing units for multi-task near-field photonic computing</title>
    <updated>2026-07-09T11:20:00Z</updated>
    <link href="https://arxiv.org/abs/2607.08360v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.08360v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Integrated photonic neural networks require optical operators that are simultaneously compact, matrix-general and compatible with task-level reconfigurability. Here we introduce a meta processing unit (MPU), an inverse-designed near-field photonic device that implements local complex matrix transformations within a shallow-etched silicon region. Each 2x2 operator occupies 9.6 umx4.8 um and is designed as a reusable passive matrix primitive that can be combined with reconfigurable MZI neurons. We demonstrate a 3-bit quantized MZI-equivalent unitary device library with an effective reconstruction precision of 3.32 bits. Beyond unitary operators, we validate arbitrary complex 2x2 matrix fitting and a cascaded 4x4 matrix operation with 92.7% fidelity. We further integrate the MPU with active photonic components and hardware-in-the-loop training, achieving test accuracies of 83.5% and 80.9% on dual-task vowel recognition. In large-scale EMNIST simulations, a fine-grained neuron-level MPU replacement strategy reaches 87.64% average accuracy at 90% shared-MPU replacement, outperforming a layer-level baseline by 7.26 percentage points. These results establish inverse-designed MPUs as compact passive matrix operators for heterogeneous, hardware-adaptive photonic neural networks.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <category term="eess.SP" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-09T11:20:00Z</published>
    <arxiv:comment>48 pages, 19 figures</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Chu Wu</name>
    </author>
    <author>
      <name>Zeyu Cai</name>
    </author>
    <author>
      <name>Songtao Yang</name>
    </author>
    <author>
      <name>Ruoyu Shen</name>
    </author>
    <author>
      <name>Yinan Zhao</name>
    </author>
    <author>
      <name>Haiou Zhang</name>
    </author>
    <author>
      <name>Wei Chu</name>
    </author>
    <author>
      <name>Xing Lin</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2607.07274v1</id>
    <title>Beyond white- and black-box modeling tools in optical communications and optical computing: physics-informed data-driven modeling</title>
    <updated>2026-07-08T11:04:54Z</updated>
    <link href="https://arxiv.org/abs/2607.07274v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2607.07274v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Efficient optimization and control of photonic computing and communication systems increasingly rely on accurate surrogate models/digital twins. While data-driven models may achieve faster inference than traditional physics-based methods, they typically suffer from poor training data efficiency and limited generalizability. To address this trade-off, physics-informed data-driven modeling has emerged as a powerful hybrid paradigm. This paper presents a comparative analysis of these three modeling paradigms across three benchmark use cases: optical amplifiers, directly modulated lasers, and interferometer meshes. By evaluating model complexity, data efficiency, generalizability, and modularity, this work provides a detailed analysis of the respective trade-offs and highlights the advantages of combining physical insight with data-driven learning.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <category term="eess.SP" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-07-08T11:04:54Z</published>
    <arxiv:comment>Submitted to Journal of Lightwave Technology</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Isidora Teofilovic</name>
    </author>
    <author>
      <name>Sergio Hernandez Fernandez</name>
    </author>
    <author>
      <name>Metodi P. Yankov</name>
    </author>
    <author>
      <name>Christophe Peucheret</name>
    </author>
    <author>
      <name>Darko Zibar</name>
    </author>
    <author>
      <name>Francesco Da Ros</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2606.26254v1</id>
    <title>A Survey of Quantum Programming Languages</title>
    <updated>2026-06-24T18:01:51Z</updated>
    <link href="https://arxiv.org/abs/2606.26254v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2606.26254v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Quantum computing has seen multiple recent breakthroughs and is getting closer to demonstrations of an exponential advantage over classical computing for certain problems. Programmers will require high-level, general-purpose, executable programming languages to express quantum solutions clearly and effectively, and the field has already produced a wide variety of such languages. This paper presents a language classification framework and uses it to survey ten popular quantum programming languages. The findings include conceptual and experimental comparisons that result in a list of challenges for future language design.</summary>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.PL" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-06-24T18:01:51Z</published>
    <arxiv:comment>27 pages, 17 figures, 6 tables</arxiv:comment>
    <arxiv:primary_category term="quant-ph"/>
    <author>
      <name>Quan Do</name>
    </author>
    <author>
      <name>Hersh Gupta</name>
    </author>
    <author>
      <name>Xiyuan Cao</name>
    </author>
    <author>
      <name>Aarav Pabla</name>
    </author>
    <author>
      <name>Pranav Singamsetty</name>
    </author>
    <author>
      <name>Evan O'Grady</name>
    </author>
    <author>
      <name>Keli Huang</name>
    </author>
    <author>
      <name>Jens Palsberg</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2606.23159v1</id>
    <title>General-Purpose Nonlinear Function Approximation via Linear Integrated Photonics</title>
    <updated>2026-06-22T11:02:40Z</updated>
    <link href="https://arxiv.org/abs/2606.23159v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2606.23159v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Photonic computing has emerged as a promising platform for accelerating artificial intelligence workloads by enabling low-latency and energy-efficient linear operations such as vector-matrix multiplication. However, scalable on-chip high-order nonlinear processing remains challenging, limiting the functional versatility of current photonic hardware. Here, we present an optoelectronic approach for approximating high-order and high-dimensional nonlinear functions. The key to this approach lies in optical random Fourier feature mapping, which transforms nonlinear function evaluation into an equivalent linear computation. This approach enables nonlinear computing within a linear photonic framework, eliminating the need for complex optical nonlinear or active materials while preserving scalability and computational throughput in a simple silicon photonic circuit. We experimentally demonstrate a broad class of nonlinear functions, including tenth-order Legendre polynomials, computationally demanding special functions (Voigt, Fermi-Dirac, and Fresnel), neural-network activation functions, two-dimensional nonlinear functions, and a 10-dimensional softmax layer. This work establishes a general and scalable strategy for nonlinear computing in photonic integrated hardware and opens a pathway toward fully functional optical accelerators for next-generation computing systems.</summary>
    <category term="cs.ET" scheme="http://arxiv.org/schemas/atom"/>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-06-22T11:02:40Z</published>
    <arxiv:comment>26 pages, 9 figures. Submitted to npj Unconventional Computing</arxiv:comment>
    <arxiv:primary_category term="cs.ET"/>
    <author>
      <name>Ayana Mizuno</name>
    </author>
    <author>
      <name>Isamu Takai</name>
    </author>
    <author>
      <name>Makoto Nakai</name>
    </author>
    <author>
      <name>Atsutaka Miyamichi</name>
    </author>
    <author>
      <name>Ryuichi Konishi</name>
    </author>
    <author>
      <name>Satoshi Sunada</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2606.16938v1</id>
    <title>Edge-Enhanced Diffractive Neural Networks Based on Spin-Multiplexed Nonlocal Metasurfaces</title>
    <updated>2026-06-15T16:39:39Z</updated>
    <link href="https://arxiv.org/abs/2606.16938v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2606.16938v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Single-layer diffractive neural networks often face classification accuracy bottlenecks due to limited wavefront modulation capabilities. Edge detection, as an optical image processing technique, extracts image contours and offers a promising way to simplify classification tasks. However, integrating edge detection and DNN-based classification on a single chip remains a challenge. Here, we propose an integrated nonlocal meta-platform that achieves all-optical edge detection and DNN-based classification via spin-multiplexing. By exploiting the dispersion properties of the nonlocal Huygens' metasurface, the co-polarized component in the output light performs momentum-space filtering for real-time edge detection. The cross-polarized component undergoes geometric phase modulation to execute image classification within the DNN. We couple quasi-bound states in the continuum and magnetic dipole resonances in crescent-shaped nanopillars, achieving a high polarization conversion efficiency of approximately $55\%$. This edge-enhanced DNN architecture significantly reduces data redundancy, elevating the classification accuracy of the single-layer network on the MNIST dataset from $64.2\%$ to $80.7\%$. Our work provides a compact, high-efficiency solution for integrated all-optical machine vision and intelligent photonic computing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <category term="physics.app-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-06-15T16:39:39Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Qianqian He</name>
    </author>
    <author>
      <name>Kenan Guo</name>
    </author>
    <author>
      <name>Jumin Qiu</name>
    </author>
    <author>
      <name>Shuyuan Xiao</name>
    </author>
    <author>
      <name>Tingting Liu</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2606.16398v1</id>
    <title>Octave bandwidth 3D-Printed Couplers for Low-Loss Thin-Film Lithium Tantalate Circuits</title>
    <updated>2026-06-15T08:36:42Z</updated>
    <link href="https://arxiv.org/abs/2606.16398v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2606.16398v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Low-loss, broadband photonic integrated circuits (PICs) are critical enablers for optical communications, photonic computing, and quantum applications. Lithium tantalate on insulator (LTOI) is an emerging photonic platform offering a wide transparency window and strong Pockels effect, and thereby enabling efficient electro-optic modulation and high data rates. Here, we present the first implementation of efficient out-of-plane polymer coupling interfaces fabricated via 3D direct laser writing for both fully etched strip and partially etched rib LTOI waveguides, achieving ultra-low coupling losses of 0.9 dB (strip) and 1.25 dB (rib) per interface. Both coupler types exhibit a 3 dB optical bandwidth spanning more than an octave from 850 nm to 1740 nm and maintain stable operation under 1 W optical input power. Combined with on-chip waveguides exhibiting propagation losses below 0.1 dB/cm, these characteristics represent a key step toward unlocking the full potential of LTOI for high-speed optical signal processing with an unprecedented degree of parallelism. In addition, the octave-spanning bandwidth enables efficient interfacing of both the fundamental and second-harmonic signals, making the platform highly attractive for second harmonic generation based quantum squeezing applications.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-06-15T08:36:42Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Erik Jung</name>
    </author>
    <author>
      <name>Xinyu Ma</name>
    </author>
    <author>
      <name>Jan Brandes</name>
    </author>
    <author>
      <name>Caghan Ünlüer</name>
    </author>
    <author>
      <name>Shabnam Taheriniya</name>
    </author>
    <author>
      <name>Seongmin Jo</name>
    </author>
    <author>
      <name>Philipp Schmidt</name>
    </author>
    <author>
      <name>Eric Biedert</name>
    </author>
    <author>
      <name>Liam McRae</name>
    </author>
    <author>
      <name>Julian Rasmus Bankwitz</name>
    </author>
    <author>
      <name>Frank Brückerhoff-Plückelmann</name>
    </author>
    <author>
      <name>Wolfram Pernice</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2606.16150v1</id>
    <title>Spatiotemporally Interleaved Homodyne Photonic Tensor Core</title>
    <updated>2026-06-15T03:11:04Z</updated>
    <link href="https://arxiv.org/abs/2606.16150v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2606.16150v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Photonic computing provides ultrahigh bandwidth, low latency and intrinsic parallelism, making it a promising route beyond the scaling limits of electronic computing. However, existing on-chip photonic computing systems remain constrained by persistent trade-offs among high-speed modulation, energy efficiency and large-scale integration, limiting their system-level advantages. Here we present a spatiotemporally interleaved homodyne photonic tensor core implemented on a thin-film lithium niobate (TFLN) platform. By integrating a homodyne photonic matrix with a bus-readout time-integrating array, this architecture scales down the high-speed digital-to-analog and electro-optic interconversion hardware overhead required for photonic matrix operations from O(n^2) to O(n), thereby unlocking system-level scalability. Moreover, the architecture employs orthogonal horizontal and vertical crossbars to route data and weight signals independently, eliminating the intrinsic beam combining loss while enabling ultrahigh-speed synchronous updates of both data and weights. Collectively, these features provide a scalable and hardware-efficient foundation for high-bandwidth photonic processors targeting general-purpose artificial intelligence (AI) computing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <category term="physics.app-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-06-15T03:11:04Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Yun-Long Nie</name>
    </author>
    <author>
      <name>Hang Song</name>
    </author>
    <author>
      <name>De-Hui Huang</name>
    </author>
    <author>
      <name>Yi Xie</name>
    </author>
    <author>
      <name>Yu-Xuan Fu</name>
    </author>
    <author>
      <name>Jian-Peng Dou</name>
    </author>
    <author>
      <name>Xiao-Yun Xu</name>
    </author>
    <author>
      <name>Hao Tang</name>
    </author>
    <author>
      <name>Xian-Min Jin</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2606.15391v1</id>
    <title>Multi-channel high-speed flip-chip packaging platform for thin-film lithium niobate photonic circuits</title>
    <updated>2026-06-13T16:41:54Z</updated>
    <link href="https://arxiv.org/abs/2606.15391v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2606.15391v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>To address the urgent need for multi-channel high-speed electrical interfacing of thin-film lithium niobate (TFLN) photonic circuits, we realize a flip-chip packaging platform capable of simultaneously delivering 13 high-speed and 32 low-speed electronic signals to a centimeter-sized TFLN chip. The platform exhibits low flip-chip bonding loss and low inter-channel crosstalk over a broad bandwidth up to 50 GHz. Leveraging this packaging platform, we demonstrate high-speed electrical interfacing with two proof-of-concept TFLN photonic circuits, namely a 2x8 optical switch and an electro-optic comb-based transmitter. The switch achieves arbitrary 8-channel routing with ~3 dB insertion loss, &lt; -20 dB crosstalk, and an equipment-limited switching time of &lt;= 34 ps. The transmitter circuit includes a 50 GHz electro-optic comb generator with 2.8-dB flatness, a tunable microring to arbitrarily filter one comb line, and a modulator for data transmission at 20 Gbit/s. The packaging platform could significantly advance large-scale TFLN circuits in optical communications, microwave photonics, and photonic computing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-06-13T16:41:54Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Zhenzheng Wang</name>
    </author>
    <author>
      <name>Xiangzhi Xie</name>
    </author>
    <author>
      <name>Yikun Chen</name>
    </author>
    <author>
      <name>Yifan Wu</name>
    </author>
    <author>
      <name>Zeyu Luo</name>
    </author>
    <author>
      <name>Hanke Feng</name>
    </author>
    <author>
      <name>Yulong Chen</name>
    </author>
    <author>
      <name>Zengyi Xu</name>
    </author>
    <author>
      <name>Zixi Wang</name>
    </author>
    <author>
      <name>Yuansong Zeng</name>
    </author>
    <author>
      <name>Mandie Huang</name>
    </author>
    <author>
      <name>Ke Zhang</name>
    </author>
    <author>
      <name>Yingxia Liu</name>
    </author>
    <author>
      <name>Cheng Wang</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2606.01616v1</id>
    <title>Manifold partitioning induced sequential optical reasoning and decision framework for photonic computing</title>
    <updated>2026-06-01T03:04:27Z</updated>
    <link href="https://arxiv.org/abs/2606.01616v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2606.01616v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Real-world data are intrinsically embedded in highly entangled manifolds, making the extraction of separable representations a central challenge for artificial intelligent (AI) systems. While optical neural networks (ONNs) offer ultrafast and energy-efficient data processing, their capacity is constrained by limited physical depth. Here, we introduce a sequential optical reasoning and decision (SORD) framework, an architecture that performs time-sequenced hierarchical inference by decomposing global tasks into coarse-to-fine steps via geometry-guided data partitioning. At each step, SORD executes small reasoning via dynamic operator selection, effectively reducing the overall task complexity without scaling up physical architecture. Experimentally, SORD enables a single-layer diffractive ONN to achieve otherwise intractable 100-class optical fiber speckle classification with 94% accuracy and a system energy efficiency of 23.3 TOPS/W. This high-fidelity recognition is further examined in a human-machine interface, featuring real-time interactive all-optical sensing. Overall, our work establishes a scalable and hardware-efficient approach to expanding the effective expressivity of compact photonic AI systems, and may advance their deployment in applications requiring real-time sensing, inference, and control.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-06-01T03:04:27Z</published>
    <arxiv:comment>25 pages, 5 figures, submitted to a journal</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Zhihao Li</name>
    </author>
    <author>
      <name>Jing Pan</name>
    </author>
    <author>
      <name>Wei Yan</name>
    </author>
    <author>
      <name>Yu Xie</name>
    </author>
    <author>
      <name>Lingmei Ma</name>
    </author>
    <author>
      <name>Xiaoyu Sun</name>
    </author>
    <author>
      <name>Min Qiu</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2605.30703v1</id>
    <title>Mid-infrared single-pixel imaging at the single-photon level</title>
    <updated>2026-05-29T00:50:45Z</updated>
    <link href="https://arxiv.org/abs/2605.30703v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2605.30703v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Single-pixel cameras have recently emerged as promising alternatives to multi-pixel sensors due to reduced costs and superior durability, which are particularly attractive for mid-infrared (MIR) imaging pertinent to applications including industry inspection and biomedical diagnosis. To date, MIR single-pixel photon-sparse imaging has yet been realized, which urgently calls for high-sensitivity optical detectors and high-fidelity spatial modulators. Here, we demonstrate a MIR single-photon computational imaging with a single-element silicon detector. The underlying methodology relies on nonlinear structured detection, where the encoded time-varying pump patterns are optically imprinted onto the MIR object image through sum-frequency generation. Simultaneously, the MIR radiation is spectrally translated into the visible region, thus permitting infrared single-photon upconversion detection. Then, the use of advanced algorithms of compress sensing and deep learning allows us to reconstruct MIR images under sub-Nyquist sampling and photon-starving illumination. The presented paradigm of single-pixel upconversion imaging is featured with single-pixel simplicity, single-photon sensitivity, and room-temperature operation, which would establish a new path for sensitive imaging at longer infrared wavelengths or terahertz frequencies, where high-sensitivity photon counters and high-fidelity spatial modulators are typically hard to access.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-05-29T00:50:45Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <arxiv:journal_ref>Nature Communications 14, 1073 (2023)</arxiv:journal_ref>
    <author>
      <name>Yinqi Wang</name>
    </author>
    <author>
      <name>Kun Huang</name>
    </author>
    <author>
      <name>Jianan Fang</name>
    </author>
    <author>
      <name>Ming Yan</name>
    </author>
    <author>
      <name>E Wu</name>
    </author>
    <author>
      <name>Heping Zeng</name>
    </author>
    <arxiv:doi>10.1038/s41467-023-36815-3</arxiv:doi>
    <link rel="related" href="https://doi.org/10.1038/s41467-023-36815-3" title="doi"/>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2605.28439v1</id>
    <title>Compile-Time Simplification of Classically Controlled Operations in Dynamic Circuits</title>
    <updated>2026-05-27T13:05:41Z</updated>
    <link href="https://arxiv.org/abs/2605.28439v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2605.28439v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Dynamic circuits use real-time outcomes of mid-circuit measurements, processed by a classical controller, to adapt subsequent operations during circuit execution. This additional flexibility over static circuits comes at a price. Mid-circuit measurements are typically slower and noisier than unitary gates. Furthermore, classical feedforward requires exchanging information between the quantum processor (QPU) and the classical controller, introducing latency that erodes the practical performance of dynamic circuits. We propose a compile-time optimization framework that reduces the use of classical controls in dynamic circuits while preserving their semantics. At its core, the framework uses a static analysis that symbolically executes the circuit by propagating classical information alongside the quantum state. By combining this classical-quantum information with the Probabilistic Circuit Model extended with probabilistic controls that emulate classical feedforward, we obtain an intermediate probabilistic representation of the dynamic circuit. In this representation, mid-circuit measurements and classically controlled operations can be removed or rewritten as purely unitary operations and probabilistic components. Compared to existing compile-time optimizations that target only mid-circuit measurements, our method applies to a broader class of dynamic circuits expressible in modern quantum programming languages. We evaluated our framework on randomly generated dynamic circuits, achieving about 50% classical feedforward reduction and even higher reductions in favorable settings.</summary>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.ET" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-05-27T13:05:41Z</published>
    <arxiv:comment>Accepted at ISC High Performance 2026; to appear in the IEEE Xplore proceedings</arxiv:comment>
    <arxiv:primary_category term="quant-ph"/>
    <author>
      <name>Innocenzo Fulginiti</name>
    </author>
    <author>
      <name>Yanbin Chen</name>
    </author>
    <author>
      <name>Christian B. Mendl</name>
    </author>
    <author>
      <name>Helmut Seidl</name>
    </author>
    <arxiv:doi>10.23919/ISC.2026.11520473</arxiv:doi>
    <link rel="related" href="https://doi.org/10.23919/ISC.2026.11520473" title="doi"/>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2605.27607v1</id>
    <title>18-dB on-chip vacuum squeezing in an adaptively poled lithium niobate waveguide</title>
    <updated>2026-05-26T19:24:01Z</updated>
    <link href="https://arxiv.org/abs/2605.27607v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2605.27607v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Quantum squeezed states of light can enhance measurement sensitivity beyond classical limits and enable quantum information processing, but scalable low-loss sources remain challenging. We demonstrate continuous-wave quantum squeezing on a chip, achieving 18 dB of squeezing and 20 dB of anti-squeezing at 1570 nm in a 1.6-cm traveling-wave adaptively poled thin-film lithium niobate waveguide. A distributed model independently determines facet losses, phase noise, and nonlinear interaction strength without prior assumptions, enabling rigorous inference of on-chip performance. We estimate a 95% confidence interval of [-18.96, -17.25] dB squeezing and [19.96, 21.35] dB anti-squeezing. These values represent the highest squeezing reported for any integrated photonic platform and the first assumption-free statistical validation of integrated squeezing performance. Our results establish thin-film lithium niobate as a high-performance, scalable platform for continuous-variable quantum sensing, communications, and photonic computing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-05-26T19:24:01Z</published>
    <arxiv:comment>17 Pages, 4 figures</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Tushar Sanjay Karnik</name>
    </author>
    <author>
      <name>Xinyi Ren</name>
    </author>
    <author>
      <name>Chun-Ho Lee</name>
    </author>
    <author>
      <name>Bo-Han Wu</name>
    </author>
    <author>
      <name>Mihir Chaudhari</name>
    </author>
    <author>
      <name>Clayton Cheung</name>
    </author>
    <author>
      <name>James Wang</name>
    </author>
    <author>
      <name>Shi-Yuan Ma</name>
    </author>
    <author>
      <name>Mahmoud Jalali Mehrabad</name>
    </author>
    <author>
      <name>Ian Christen</name>
    </author>
    <author>
      <name>Reshma Kopparapu</name>
    </author>
    <author>
      <name>Kiwon Kwon</name>
    </author>
    <author>
      <name>Yue Yu</name>
    </author>
    <author>
      <name>Sri Krishna Vadlamani</name>
    </author>
    <author>
      <name>Kamila Kunes</name>
    </author>
    <author>
      <name>Quntao Zhuang</name>
    </author>
    <author>
      <name>Dirk Englund</name>
    </author>
    <author>
      <name>Zaijun Chen</name>
    </author>
    <author>
      <name>Mengjie Yu</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2605.25336v1</id>
    <title>Mid-infrared single-photon computational temporal ghost imaging</title>
    <updated>2026-05-25T01:40:18Z</updated>
    <link href="https://arxiv.org/abs/2605.25336v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2605.25336v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>The capture of transient optical waveforms is critical to reveal dynamical phenomena in various fields. However, fast and sensitive mid-infrared (MIR) measurements are typically limited by processing bandwidth and detection sensitivity of conventional infrared detectors. Here, we propose and implement a computational temporal ghost imaging system, which favors high-speed and high-sensitivity characterization of MIR temporal objects. The core process relies on high-fidelity nonlinear optical transduction for facilitating both the programmable structured illumination and frequency upconversion detection based on the high-performance near-infrared light modulator and detector, respectively. Consequently, the correlation between the recorded integral upconversion intensity and the designated encoding patterns allows one to reconstruct the MIR profiles with a temporal resolution of 80 ps, well beyond the intrinsic bandwidth or timing jitter of the involved detectors. Moreover, a record-high detection sensitivity is manifested by recovering single-photon MIR waveforms with an incident flux below 0.1 photon/bit. Additionally, faithful reconstructions at sub-Nyquist sampling rates are demonstrated using the compressive sensing algorithm, which can reduce the data acquisition time by over 90\%. The presented paradigm features high timing precision, single-photon sensitivity, and efficient data sampling, which could be extended into far-infrared or terahertz regions to address pressing demands in fast and sensitive sensing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-05-25T01:40:18Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <arxiv:journal_ref>Laser &amp; Photonics Reviews 19, 2402180 (2025)</arxiv:journal_ref>
    <author>
      <name>Wen Zhang</name>
    </author>
    <author>
      <name>Kun Huang</name>
    </author>
    <author>
      <name>Xu Wang</name>
    </author>
    <author>
      <name>Ben Sun</name>
    </author>
    <author>
      <name>Jianan Fang</name>
    </author>
    <author>
      <name>Yijing Li</name>
    </author>
    <author>
      <name>Heping Zeng</name>
    </author>
    <arxiv:doi>10.1002/lpor.202402180</arxiv:doi>
    <link rel="related" href="https://doi.org/10.1002/lpor.202402180" title="doi"/>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2605.23051v1</id>
    <title>General-Purpose Photonic Computing Primitive for Contemporary Artificial Intelligence</title>
    <updated>2026-05-21T21:33:59Z</updated>
    <link href="https://arxiv.org/abs/2605.23051v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2605.23051v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Photonic computing offers a promising route to accelerating artificial intelligence (AI) by providing high analog bandwidth, low latency, and low energy consumption. However, existing optical neural networks (ONNs) struggle with substantial hardware overhead and limited support for the dynamic, arbitrary matrix operations essential for modern AI architectures. Here we present the dynamic universal encoding tensorcore (DUET), a general-purpose photonic computing paradigm based on vectorized operand differential interferometric cells (VODICs). By exploiting inherent structural symmetry, this design provides a full-range linear encoding interface that directly accommodates signed operands. This approach eliminates the sign-based path splitting, nonlinear remapping, and auxiliary preprocessing typically required in conventional ONNs, thereby reducing latency and minimizing hardware and memory overhead. We further implement a hardware-aware training (HAT) strategy to alleviate the impact of on-chip non-idealities and ensure stable inference. DUET is experimentally validated across diverse architectures and application domains, ranging from image classification and medical segmentation to Transformer-based content generation, demonstrating competitive performance. By extending optical computing to universal, full-range operators across diverse model architectures, DUET provides a viable pathway toward general-purpose optical acceleration for contemporary AI workloads.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <category term="physics.app-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-05-21T21:33:59Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Shupeng Ning</name>
    </author>
    <author>
      <name>Chenghao Feng</name>
    </author>
    <author>
      <name>Zhenxiang Xu</name>
    </author>
    <author>
      <name>Hanqing Zhu</name>
    </author>
    <author>
      <name>David Z. Pan</name>
    </author>
    <author>
      <name>Jiaqi Gu</name>
    </author>
    <author>
      <name>Ray T. Chen</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2605.20864v1</id>
    <title>Scalable native signed optical computing enabled by dual-wavelength incoherent multiplexing</title>
    <updated>2026-05-20T07:56:08Z</updated>
    <link href="https://arxiv.org/abs/2605.20864v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2605.20864v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Incoherent photonic neural networks (PNNs) provide a robust platform for analog optical computing, yet efficient implementation of native signed operations remains challenging. Existing incoherent PNNs approaches often require additional spatial channels or temporal encoding steps to represent bipolar input signals, resulting in hardware overhead that scales with system size. Here, we demonstrate a dual-wavelength incoherent photonic architecture that natively supports both signed inputs and signed weights on a thin-film lithium niobate platform. By encoding complementary signal components onto two wavelength channels and performing computation within a shared physical path, the proposed scheme eliminates duplicated weighting units. As a result, the additional hardware overhead associated with signed computation remains constant per multiply accumulate operation, independent of matrix size. The fabricated device exhibits a modulation bandwidth exceeding 40 GHz and achieves four-quadrant optical multiplication with a standard deviation error of 1.27%. System-level functionality is validated through neural-network classification, achieving 95.1% accuracy on the Moons dataset and 91.63% on MNIST. These results establish a practical route toward scalable incoherent photonic computing systems with native bipolar processing capability.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-05-20T07:56:08Z</published>
    <arxiv:comment>13 pages, 4 figures</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Yuan Ren</name>
    </author>
    <author>
      <name>Yong Zheng</name>
    </author>
    <author>
      <name>Ruixue Liu</name>
    </author>
    <author>
      <name>Yunpeng Song</name>
    </author>
    <author>
      <name>Qinfen Huang</name>
    </author>
    <author>
      <name>Min Wang</name>
    </author>
    <author>
      <name>Ya Cheng</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2605.20768v1</id>
    <title>Mid-infrared single-photon sub-pixel temporal ghost imaging</title>
    <updated>2026-05-20T06:11:29Z</updated>
    <link href="https://arxiv.org/abs/2605.20768v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2605.20768v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Temporal ghost imaging (TGI) enables ultrafast temporal signal recovery using slow detectors, offering a promising route for high-speed mid-infrared (MIR) detection. However, conventional schemes remain limited in temporal resolution by the modulation bandwidth or pattern timescale, and are mostly confined to structured illumination. Here, we demonstrated a high-resolution MIR single-photon computational TGI system, which integrated nonlinear structured detection with sub-pixel temporal shifting. A pre-programmed near-infrared pump serves as a temporally optical gate to drive sum-frequency generation in a nonlinear crystal. Consequently, MIR waveforms at 3.4 $μ$m were upconverted, and captured by a room-temperature silicon detector. We realized sub-pixel operation by fractional-bin temporal stepping of the gate and multi-shot fusion via pseudo-inverse reconstruction. The sub-pixel shifting strategy decouples the achievable resolution from modulation speed, enabling 40 ps temporal precision at a driving rate of only 3.125 Gbps. This performance surpasses both detector jitter and pattern-rate limits, while maintaining single-photon sensitivity. The presented paradigm establishes a versatile route for ultrafast MIR waveform reconstruction, opening new opportunities in high-resolution infrared sensing and quantum photonics.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-05-20T06:11:29Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <arxiv:journal_ref>Laser &amp; Photonics Reviews 20, e02587 (2026)</arxiv:journal_ref>
    <author>
      <name>Wen Zhang</name>
    </author>
    <author>
      <name>Kun Huang</name>
    </author>
    <author>
      <name>Zhibin Zhao</name>
    </author>
    <author>
      <name>Huijie Ma</name>
    </author>
    <author>
      <name>Ziyu He</name>
    </author>
    <author>
      <name>Jianan Fang</name>
    </author>
    <author>
      <name>Heping Zeng</name>
    </author>
    <arxiv:doi>10.1002/lpor.202502587</arxiv:doi>
    <link rel="related" href="https://doi.org/10.1002/lpor.202502587" title="doi"/>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2605.19152v2</id>
    <title>Information Processing Capacity of Stationary Physical Systems: Theory, Data-efficient Estimation Methods, and Photonic Demonstration</title>
    <updated>2026-05-21T13:18:25Z</updated>
    <link href="https://arxiv.org/abs/2605.19152v2" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2605.19152v2" rel="related" type="application/pdf" title="pdf"/>
    <summary>Physical computing systems provide a promising route toward hardware-native machine learning, but their computational capabilities remain difficult to characterize in a principled, task-independent, and data-efficient way. We extend the Information Processing Capacity (IPC) framework to stationary physical computing systems and establish several fundamental results: individual capacities are bounded between zero and one, their sum over a complete basis is bounded by the number of readouts, and noise strictly reduces this bound. We address the finite-sample estimation of IPC and derive the asymptotic form of the systematic positive bias affecting naive estimators. Building on these results, we introduce data-efficient estimation methods based on Richardson extrapolation and Sobol quasi-random sampling. We validate the framework experimentally using a photonic computing system based on picosecond laser pulses propagating through a nonlinear optical fibre. By varying the laser power and fibre length, we observe systematic shifts of the IPC distribution toward higher-order nonlinear capacities induced by the Kerr effect. Finally, we demonstrate that the total IPC strongly correlates with performance on benchmark machine-learning tasks and provides a reliable estimate of the effective dimensionality of the system. These results establish IPC as a practical bridge between the intrinsic dynamics of physical computing systems and their machine-learning performance.</summary>
    <category term="stat.ML" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.ET" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.IT" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.LG" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.NE" scheme="http://arxiv.org/schemas/atom"/>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-05-18T22:13:52Z</published>
    <arxiv:comment>added 2 new references</arxiv:comment>
    <arxiv:primary_category term="stat.ML"/>
    <author>
      <name>Rahul Uma Ramachandran</name>
    </author>
    <author>
      <name>Serge Massar</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2605.14690v2</id>
    <title>Integrated photonic computing: towards high-dimensional information processing</title>
    <updated>2026-05-16T21:31:04Z</updated>
    <link href="https://arxiv.org/abs/2605.14690v2" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2605.14690v2" rel="related" type="application/pdf" title="pdf"/>
    <summary>The rapid growth of artificial intelligence, coupled with the slowing of Moore's law, is straining computing infrastructure, as CMOS electronics face inherent limits in bandwidth, energy efficiency, and parallelism. Integrated photonic computing encodes and processes information using the phase, amplitude, spatial modes, wavelength channels, and polarisation of guided optical fields, offering a scalable and energy-efficient route beyond charge-based signalling. Here, we review on-chip photonic computing, emphasising the progression from low-dimensional to high-dimensional architectures. At the foundational level, low-dimensional approaches manipulate the phase and amplitude of guided light through Mach-Zehnder interferometers, diffractive structures, microring resonators, and absorptive elements, forming a programmable basis for optical matrix-vector multiplication. Crucially, high-dimensional architectures exploit spatial modes and wavelength channels to carry multiple independent data streams through a single waveguide, achieving higher throughput with moderate hardware overhead. Practical deployment, however, demands more than device innovation. We examine how system-level techniques, from time-wavelength interleaving to hardware-aware training, address energy efficiency, precision, and algorithm-hardware co-design. Five challenges nevertheless remain: electro-optic conversion efficiency, computing parallelism, spatial integration, reconfigurability, and robustness. We highlight emerging topological structures, such as optical skyrmions, as a promising route to fault-tolerant, topologically protected encoding that exploits the largely untapped polarisation degree of freedom. We argue that, by embracing the higher dimensionality of light, photonic computing can offer not merely an incremental improvement but a new paradigm for high-performance, energy-efficient information processing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-05-14T11:03:29Z</published>
    <arxiv:comment>22 pages, 7 figures</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Ji Qin</name>
    </author>
    <author>
      <name>Zhi-Kai Pong</name>
    </author>
    <author>
      <name>Xuke Qiu</name>
    </author>
    <author>
      <name>Liangyu Deng</name>
    </author>
    <author>
      <name>Runchen Zhang</name>
    </author>
    <author>
      <name>Yunqi Zhang</name>
    </author>
    <author>
      <name>Jinge Guo</name>
    </author>
    <author>
      <name>Yifei Ma</name>
    </author>
    <author>
      <name>Zimo Zhao</name>
    </author>
    <author>
      <name>Yuanxing Shen</name>
    </author>
    <author>
      <name>Patrick Salter</name>
    </author>
    <author>
      <name>Martin Booth</name>
    </author>
    <author>
      <name>Stephen Morris</name>
    </author>
    <author>
      <name>Honghui He</name>
    </author>
    <author>
      <name>Min Gu</name>
    </author>
    <author>
      <name>Bowei Dong</name>
    </author>
    <author>
      <name>Chao He</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2604.24541v1</id>
    <title>Noise in analog programmable-photonic computation</title>
    <updated>2026-04-27T14:37:19Z</updated>
    <link href="https://arxiv.org/abs/2604.24541v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2604.24541v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Analog Programmable-Photonic Computation (APC) leverages programmable integrated photonics (PIP) to perform high-speed matrix operations using optical waves. However, the continuous nature of optical waves that implement the analog bits or anbits - the fundamental unit of information in APC - makes computational results intrinsically sensitive to physical noise. Here, we establish and experimentally validate a comprehensive noise analysis in APC platforms using the geometric representation of the anbit in the Generalized Bloch Sphere (GBS). By modeling the physical noise sources in PIP circuits as random photocurrent fluctuations at the output of the opto-electrical (O/E) converter, and using error propagation theory, the noise statistics can be projected onto the GBS. This approach leads to specific noise maps in the GBS for each noise source, enabling the identification of the dominant noise sources within the APC system. Analytical predictions are numerically and experimentally validated on a fabricated silicon PIP chip. Beyond statistical characterization of system noise, the proposed model provides quantitative design criteria for noise-adapted analog constellations in the GBS, advancing APC towards scalable and robust optical computing systems, with potential applications in emerging paradigms such as photonic neuromorphic computing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-04-27T14:37:19Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Raúl López-March</name>
    </author>
    <author>
      <name>Andrés Macho-Ortiz</name>
    </author>
    <author>
      <name>Francisco Javier Fraile-Peláez</name>
    </author>
    <author>
      <name>José Capmany</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2604.22660v1</id>
    <title>Fully multiplexed photonic tensor computing</title>
    <updated>2026-04-24T15:35:54Z</updated>
    <link href="https://arxiv.org/abs/2604.22660v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2604.22660v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Tensor operations dominate modern computational workloads, yet their further acceleration demands hardware platforms with greater parallelism. Although photonic computing provides a compelling route for parallel processing, fully exploiting all native multiplexing dimensions of optical fields is impeded by the challenges in routing and programming light in all dimensions simultaneously. Here we introduce FieldCore, a fully multiplexed photonic tensor core that jointly harnesses wavelength, radio-frequency, guided-mode, time and space dimensions, thereby enabling parallelism to scale multiplicatively within a single optical field. Enabled by inverse-designed silicon photonics, FieldCore preserves a uniform programmed computation across all multiplexed channels in parallel. Experimentally, we validate and benchmark its performance from ultra-high-baudrate arithmetic operations to high-fidelity image convolution and parallel handwritten-digit recognition. We further use FieldCore to unlock applications that naturally require high-dimensional data processing, such as high-dimensional hyperspectral classification and massively parallel mechanical fault diagnosis. Our FieldCore supports an estimated aggregate compute throughput of 69.12 tera operations per second (TOPS) and accommodates up to 1,800 parallel input streams within a single core, establishing a scalable paradigm for fully multiplexed photonic tensor computing and AI inference.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-04-24T15:35:54Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Aolong Sun</name>
    </author>
    <author>
      <name>Junhao Zhao</name>
    </author>
    <author>
      <name>Fangchen Hu</name>
    </author>
    <author>
      <name>Sizhe Xing</name>
    </author>
    <author>
      <name>Yuqin Yuan</name>
    </author>
    <author>
      <name>Jialin He</name>
    </author>
    <author>
      <name>Yongzhu Hu</name>
    </author>
    <author>
      <name>Xuyu Deng</name>
    </author>
    <author>
      <name>Yinjun Liu</name>
    </author>
    <author>
      <name>Ouhan Huang</name>
    </author>
    <author>
      <name>Baiheng Zhao</name>
    </author>
    <author>
      <name>Hancheng Liu</name>
    </author>
    <author>
      <name>Tian Dong</name>
    </author>
    <author>
      <name>Jingkai Zhou</name>
    </author>
    <author>
      <name>Haoyang Sun</name>
    </author>
    <author>
      <name>Liang Chen</name>
    </author>
    <author>
      <name>Chao Shen</name>
    </author>
    <author>
      <name>Feng Bao</name>
    </author>
    <author>
      <name>Ziwei Li</name>
    </author>
    <author>
      <name>Jianyang Shi</name>
    </author>
    <author>
      <name>Wei Chu</name>
    </author>
    <author>
      <name>Bowei Dong</name>
    </author>
    <author>
      <name>Nan Chi</name>
    </author>
    <author>
      <name>Junwen Zhang</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2604.21656v1</id>
    <title>Speed-oriented quantum circuit backend</title>
    <updated>2026-04-23T13:19:34Z</updated>
    <link href="https://arxiv.org/abs/2604.21656v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2604.21656v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>We present a new software package for efficient quantum circuit generation, designed to achieve optimal runtime performance. Despite being in an early stage of development, our implementation demonstrates significant advantages over existing tools. Using the quantum Fourier transform (QFT) as a benchmark, we show that our backend can generate circuits for systems with up to 2000 qubits faster than widely used frameworks such as Qiskit and Q#. This improvement is particularly relevant for applications where classical preprocessing time, including circuit generation, must be minimized to not diminish any potential quantum advantage - for example, in combinatorial optimization tasks. Additionally, our software provides high-level primitives for bit- and integer-level manipulations, offering a simplified interface for integration with high-level quantum programming languages.</summary>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-04-23T13:19:34Z</published>
    <arxiv:comment>7 pages, 5 figures</arxiv:comment>
    <arxiv:primary_category term="quant-ph"/>
    <author>
      <name>Sören Wilkening</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2604.18496v2</id>
    <title>Homodyne Photonic Tensor Processor exceeds 1,000-TOPS</title>
    <updated>2026-04-21T03:15:05Z</updated>
    <link href="https://arxiv.org/abs/2604.18496v2" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2604.18496v2" rel="related" type="application/pdf" title="pdf"/>
    <summary>High-performance computing underpins modern artificial intelligence (AI), enabling foundation models, real-time inference and perception in autonomous systems, and data-intensive scientific simulations. Recent advances in quantization techniques utilizing low-precision computation without degrading model accuracy, create new opportunities for analog photonic computing characterized by ultra-high clock rates and low energy consumption. Here we propose and demonstrate a coherent homodyne integrated circuit capable of general matrix multiplication (GEMM) with aggregate throughput that exceeds 1,000 TOPS (tera-operations per second), enabled by massive on-chip optical fanout and parallelism. By leveraging time multiplexing, the required modulator count is reduced from O($N^2$) to O(N), allowing dense integration of record-scale 256 $\times$ 256 homodyne units (each &lt;0.0064 $mm^2$) within a single reticle. We employ wafer-scale fabricated 64 thin-film lithium niobate (TFLN) transmitters (each over 40-GHz bandwidth with propagation loss of 0.2 dB/cm) to encode data and chip-to-chip coupled to Si/SiN computing circuits (64 channels). Our system achieves up to 7-bit computational accuracy across 8 $\times$ 8 parallel channels at record computing clockrate 120 Gbaud/s, and 6-bit statistical accuracy across 256 $\times$ 100 channels at 20-128 Gbaud/s, representing a total throughput of 1,000-6,000 TOPS. Massive parallelism amortizes the optoelectronic (OE) conversion to allow 330-TOPS/W efficiency using foundry-available packaging technology. The system throughput is benchmarked with Qwen2.5-0.5 billion parameter models that generate accurate tokens. High throughput and energy efficiency establish a near-term pathway toward light-based accelerators for large-scale training and low-latency inference from datacenters to edges, accelerating new models toward artificial general intelligence.</summary>
    <category term="cs.ET" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-04-20T16:44:56Z</published>
    <arxiv:primary_category term="cs.ET"/>
    <author>
      <name>Lian Zhou</name>
    </author>
    <author>
      <name>Kaiwen Xue</name>
    </author>
    <author>
      <name>Yun-Jhu Lee</name>
    </author>
    <author>
      <name>Chun-Ho Lee</name>
    </author>
    <author>
      <name>Yuan Li</name>
    </author>
    <author>
      <name>Kiwon Kwon</name>
    </author>
    <author>
      <name>Weipeng Zhang</name>
    </author>
    <author>
      <name>Songlin Zhao</name>
    </author>
    <author>
      <name>Jason Moraes</name>
    </author>
    <author>
      <name>Niranjan Bhatia</name>
    </author>
    <author>
      <name>Ryan Hamerly</name>
    </author>
    <author>
      <name>Mengjie Yu</name>
    </author>
    <author>
      <name>Zaijun Chen</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2604.13450v1</id>
    <title>Distributed Coherent Optical Computing via Injection-Locked Photonic Networks</title>
    <updated>2026-04-15T04:03:07Z</updated>
    <link href="https://arxiv.org/abs/2604.13450v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2604.13450v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Coherent photonic computing uses both the phase and amplitude of light to implement linear operations such as dot products and matrix multiplication but requires phase stability between the interfering paths. This poses a challenge for such strategies when optical data is generated at a remote source due to environmental phase variations in fiber. Conventional approaches to distributed computing rely on optical-to-electrical conversion and buffering, limiting truly real-time and distributed computation. Here, we propose a new strategy via optical injection locking to enable distributed, real-time coherent optical processing without unnecessary conversions in the optical-to-electrical or analog-to-digital domains. Using a semiconductor laser rate-equation model, we explore the conditions required for stable operation by sweeping the power injection ratio, frequency detuning, and modulation conditions of the remote and injected lasers. Our results indicate that higher injection powers broaden the locking margin but more readily exhibit frequency-selective features associated with relaxation oscillations and increased amplitude-phase mixing, whereas lower injection powers yield a narrower, but more predictable operating window which remains stable under large modulation depth. End-to-end symbol-sequence simulations with balanced detection and temporal integration further confirm that reducing the injection ratio suppresses residual remote-modulation components in the injected laser output and improves computational accuracy. Overall, our study provides guidance and design trade-offs for remote coherent detection and distributed coherent photonic computing enabled by injection locking.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-04-15T04:03:07Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Shenghan Gao</name>
    </author>
    <author>
      <name>Kathy Lüdge</name>
    </author>
    <author>
      <name>Francesco Da Ros</name>
    </author>
    <author>
      <name>Nathan Youngblood</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2604.12278v1</id>
    <title>LightMat-HP: A Photonic-Electronic System for Accelerating General Matrix Multiplication With Configurable Precision</title>
    <updated>2026-04-14T04:44:05Z</updated>
    <link href="https://arxiv.org/abs/2604.12278v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2604.12278v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Matrix multiplication is a fundamental kernel in large-scale artificial intelligence and scientific computing, but its performance on conventional electronic accelerators is increasingly constrained by memory bandwidth and energy efficiency. Photonic computing offers a promising alternative due to its ultra-high bandwidth, massive parallelism, and low power dissipation. However, most existing photonic systems are limited to low-precision computation because of analog optical modulation constraints and noise accumulation, which restricts their applicability in precision-critical workloads. To address this limitation, we propose LightMat-HP, a hybrid photonic-electronic computing system that enables end-to-end acceleration of general matrix multiplication with configurable computational precision. LightMat-HP adopts block floating-point (BFP) arithmetic to reduce computational complexity while enabling flexible precision-performance tradeoffs. To overcome the precision limitations of photonic devices, we propose a slicing-based photonic multiplication scheme that exploits the high accuracy of low bit-width photonic multiplication in combination with digital accumulation to achieve high-precision mantissa multiplication. A tile-based matrix multiplication dataflow is further designed to support matrices of arbitrary sizes. We experimentally validate LightMat-HP on a photonic computing prototype and evaluate its performance through large-scale simulations. The results demonstrate that LightMat-HP outperforms FPGA, GPU, and a state-of-the-art photonic accelerator across throughput, latency, and energy efficiency, particularly for small- and medium-sized matrix multiplications, owing to its highly parallel photonic architecture, efficient data movement, and slice-based BFP arithmetic.</summary>
    <category term="cs.ET" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-04-14T04:44:05Z</published>
    <arxiv:comment>28 pages</arxiv:comment>
    <arxiv:primary_category term="cs.ET"/>
    <author>
      <name>Hailong Gong</name>
    </author>
    <author>
      <name>Haibo Zhang</name>
    </author>
    <author>
      <name>Amanda S. Barnard</name>
    </author>
    <author>
      <name>Mahbub Hassan</name>
    </author>
    <author>
      <name>Matt Woolley</name>
    </author>
    <author>
      <name>Rajkumar Buyya</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2604.10841v1</id>
    <title>Harnessing Photonics for Machine Intelligence</title>
    <updated>2026-04-12T22:23:14Z</updated>
    <link href="https://arxiv.org/abs/2604.10841v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2604.10841v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>The exponential growth of machine-intelligence workloads is colliding with the power, memory, and interconnect limits of the post-Moore era, motivating compute substrates that scale beyond transistor density alone. Integrated photonics is emerging as a candidate for artificial intelligence (AI) acceleration by exploiting optical bandwidth and parallelism to reshape data movement and computation. This review reframes photonic computing from a circuits-and-systems perspective, moving beyond building-block progress toward cross-layer system analysis and full-stack design automation. We synthesize recent advances through a bottleneck-driven taxonomy that delineates the operating regimes and scaling trends where photonics can deliver end-to-end sustained benefits. A central theme is cross-layer co-design and workload-adaptive programmability to sustain high efficiency and versatility across evolving application domains at scale. We further argue that Electronic-Photonic Design Automation (EPDA) will be pivotal, enabling closed-loop co-optimization across simulation, inverse design, system modeling, and physical implementation. By charting a roadmap from laboratory prototypes to scalable, reproducible electronic-photonic ecosystems, this review aims to guide the CAS community toward an automated, system-centric era of photonic machine intelligence.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.AI" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.AR" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.ET" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.LG" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-04-12T22:23:14Z</published>
    <arxiv:comment>20 pages</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Hanqing Zhu</name>
    </author>
    <author>
      <name>Shupeng Ning</name>
    </author>
    <author>
      <name>Hongjian Zhou</name>
    </author>
    <author>
      <name>Ziang Yin</name>
    </author>
    <author>
      <name>Ray T. Chen</name>
    </author>
    <author>
      <name>Jiaqi Gu</name>
    </author>
    <author>
      <name>David Z. Pan</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2604.09759v1</id>
    <title>Sustainable Transformer Neural Network Acceleration with Stochastic Photonic Computing</title>
    <updated>2026-04-10T17:18:26Z</updated>
    <link href="https://arxiv.org/abs/2604.09759v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2604.09759v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Transformers achieve state-of-the-art performance in natural language processing, vision, and scientific computing, but demand high computation and memory. To address these challenges, we present ASTRA, the first silicon-photonic accelerator leveraging stochastic computing for transformers. ASTRA employs novel optical stochastic multipliers and unary/analog homodyne accumulation in a crosstalk-minimal organization to efficiently process dynamic tensor computations. Evaluations show at least 7.6x speedup and 1.3x lower energy overheads compared to state-of-the-art accelerators, highlighting ASTRA's potential for efficient, scalable, and sustainable transformer inference.</summary>
    <category term="cs.AR" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.LG" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-04-10T17:18:26Z</published>
    <arxiv:primary_category term="cs.AR"/>
    <author>
      <name>S. Afifi</name>
    </author>
    <author>
      <name>O. Alo</name>
    </author>
    <author>
      <name>I. Thakkar</name>
    </author>
    <author>
      <name>S. Pasricha</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2604.04330v1</id>
    <title>Light-Bound Transformers: Hardware-Anchored Robustness for Silicon-Photonic Computer Vision Systems</title>
    <updated>2026-04-06T00:42:20Z</updated>
    <link href="https://arxiv.org/abs/2604.04330v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2604.04330v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Deploying Vision Transformers (ViTs) on near-sensor analog accelerators demands training pipelines that are explicitly aligned with device-level noise and energy constraints. We introduce a compact framework for silicon-photonic execution of ViTs that integrates measured hardware noise, robust attention training, and an energy-aware processing flow. We first characterize bank-level noise in microring-resonator (MR) arrays, including fabrication variation, thermal drift, and amplitude noise, and convert these measurements into closed-form, activation-dependent variance proxies for attention logits and feed-forward activations. Using these proxies, we develop Chance-Constrained Training (CCT), which enforces variance-normalized logit margins to bound attention rank flips, and a noise-aware LayerNorm that stabilizes feature statistics without changing the optical schedule. These components yield a practical ``measure $\rightarrow$ model $\rightarrow$ train $\rightarrow$ run'' pipeline that optimizes accuracy under noise while respecting system energy limits. Hardware-in-the-loop experiments with MR photonic banks show that our approach restores near-clean accuracy under realistic noise budgets, with no in-situ learning or additional optical MACs.</summary>
    <category term="cs.ET" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-04-06T00:42:20Z</published>
    <arxiv:comment>Accepted at Design Automation Conference (DAC) 2026</arxiv:comment>
    <arxiv:primary_category term="cs.ET"/>
    <author>
      <name>Xuming Chen</name>
    </author>
    <author>
      <name>Deniz Najafi</name>
    </author>
    <author>
      <name>Chengwei Zhou</name>
    </author>
    <author>
      <name>Pietro Mercati</name>
    </author>
    <author>
      <name>Arman Roohi</name>
    </author>
    <author>
      <name>Mohsen Imani</name>
    </author>
    <author>
      <name>Mahdi Nikdast</name>
    </author>
    <author>
      <name>Shaahin Angizi</name>
    </author>
    <author>
      <name>Gourav Datta</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2604.03830v1</id>
    <title>All-optical control of nonlinear emission from resonant metasurfaces</title>
    <updated>2026-04-04T19:03:13Z</updated>
    <link href="https://arxiv.org/abs/2604.03830v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2604.03830v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Nonlinear optics underpins a broad range of photonic technologies, from classical and quantum light sources to emerging nonlinear photonic neural networks. Yet, conventional nonlinear optical devices exhibit static functionality: their transfer characteristics and emission profiles are dictated by the intrinsic nonlinear process and locked by fabrication, limiting adaptability. Here, we introduce an ultra-thin metasurface platform that enables dynamic reconfiguration of nonlinear functionality in a contact-less fashion. By leveraging all-optical control of the optical torque exerted on liquid crystal molecules infiltrating a resonant metasurface, we achieve tunable polynomial nonlinear transfer functions based on third-harmonic generation process. This mechanism further allows real-time modulation of nonlinear weighting across different diffraction orders, revealing a previously unexplored interplay between mode structure and nonlinear emission. Our approach opens up a pathway toward field-programmable nonlinear photonic systems, offering unprecedented flexibility for reconfigurable nonlinear signal processing and adaptive photonic computing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-04-04T19:03:13Z</published>
    <arxiv:comment>29 pages, 6 figures, article</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Ziwei Yang</name>
    </author>
    <author>
      <name>Lei Xu</name>
    </author>
    <author>
      <name>Gabriel Sanderson</name>
    </author>
    <author>
      <name>Akhshay Bhadwal</name>
    </author>
    <author>
      <name>Luyao Wang</name>
    </author>
    <author>
      <name>Katsuya Tanaka</name>
    </author>
    <author>
      <name>Muyi Yang</name>
    </author>
    <author>
      <name>Mingkai Liu</name>
    </author>
    <author>
      <name>Shaun Lung</name>
    </author>
    <author>
      <name>Isabelle Staude</name>
    </author>
    <author>
      <name>Thomas Pertsch</name>
    </author>
    <author>
      <name>Carl Brown</name>
    </author>
    <author>
      <name>Mohsen Rahmani</name>
    </author>
    <author>
      <name>Dragomir Neshev</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2603.22811v1</id>
    <title>Toward scalable and bias-stable optical phased arrays on lithium tantalate</title>
    <updated>2026-03-24T05:18:53Z</updated>
    <link href="https://arxiv.org/abs/2603.22811v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2603.22811v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Ferroelectric materials are an ideal platform for high-speed reconfigurable photonic integrated circuits (PICs) for classical and quantum photonic computations, communications, and sensing. Most reconfigurable PIC devices achieve their functionalities via interference and are therefore highly sensitive to phase errors. Under static bias, carrier drift in ferroelectric waveguides induces continuous phase drift, creating a severe bottleneck for both PIC functionality and scalability. Here we propose achieving bias-stable and scalable ferroelectric PICs by exploiting the intrinsically low carrier drift of lithium tantalate (LT). Taking one of the PIC devices that is most sensitive to phase drift, the optical phased array (OPA), as an example, we designed and fabricated an integrated LT OPA that can keep the far-field main lobe 8 dB higher than side lobes for over 4 hours, representing at least a two-order-of-magnitude improvement over the state of the art. We demonstrated our device's capability in generating arbitrary spatiotemporal waveforms with a modulation frequency as low as 0.1 Hz, leading to practical applications in optical tweezers, trapped-ion quantum computers, adaptive optics for astronomy, AR, 3D printers, LiDAR, and free-space optical communications. Beyond OPA, our work establishes LT as a bias-stable, scalable, and high-speed PIC platform for large-scale classical and quantum photonic systems.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-03-24T05:18:53Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Gongcheng Yue</name>
    </author>
    <author>
      <name>Xuqiang Wang</name>
    </author>
    <author>
      <name>Yihan Miao</name>
    </author>
    <author>
      <name>Bowen Chen</name>
    </author>
    <author>
      <name>Yangming Zhan</name>
    </author>
    <author>
      <name>Weiran Zhou</name>
    </author>
    <author>
      <name>Phatham loahavilai</name>
    </author>
    <author>
      <name>Jiachen Cai</name>
    </author>
    <author>
      <name>Siyuan Yu</name>
    </author>
    <author>
      <name>Chengli Wang</name>
    </author>
    <author>
      <name>Xin Ou</name>
    </author>
    <author>
      <name>Yang Li</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2603.18468v2</id>
    <title>Multiscale simulations guided advances for all-optical phase-change waveguides</title>
    <updated>2026-04-10T01:22:08Z</updated>
    <link href="https://arxiv.org/abs/2603.18468v2" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2603.18468v2" rel="related" type="application/pdf" title="pdf"/>
    <summary>Photonic computing using chalcogenide phase-change materials (PCMs) is under active development for energy-efficient artificial intelligence (AI) applications. A key requirement is to enable as many optically programmable levels per device as possible, while maintaining relatively low optical loss. In this work, we carry out multiscale simulations using density functional theory and finite-difference time-domain methods, proposing a "the shorter the better" strategy to optimize the performance of Sb2Te photonic waveguide devices. Our subsequent experimental characterizations of Sb2Te thin films and optical device measurements fully verify our theoretical predictions. In particular, we reveal the unconventional optical properties of metastable crystalline Sb2Te, and utilize these features for device design, yielding a simultaneous improvement in both the programming window and the optical loss. Overall, an optical programming precision exceeding 7-bit is achieved using a single waveguide cell, setting a new record for all-optical phase-change memory devices. Our work serves as a compelling example of computational material design, which demonstrates the predictive power of multiscale simulations in guiding the design of phase-change photonic devices for enhanced performance.</summary>
    <category term="cond-mat.mtrl-sci" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-03-19T04:04:35Z</published>
    <arxiv:comment>21 pages, 8 figures</arxiv:comment>
    <arxiv:primary_category term="cond-mat.mtrl-sci"/>
    <author>
      <name>Hanyi Zhang</name>
    </author>
    <author>
      <name>Wanting Ma</name>
    </author>
    <author>
      <name>Wen Zhou</name>
    </author>
    <author>
      <name>Xueqi Xing</name>
    </author>
    <author>
      <name>Junying Zhang</name>
    </author>
    <author>
      <name>Tiankuo Huang</name>
    </author>
    <author>
      <name>Ding Xu</name>
    </author>
    <author>
      <name>Xiaozhe Wang</name>
    </author>
    <author>
      <name>Riccardo Mazzarello</name>
    </author>
    <author>
      <name>En Ma</name>
    </author>
    <author>
      <name>Jiang-Jing Wang</name>
    </author>
    <author>
      <name>Wei Zhang</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2603.15836v2</id>
    <title>Programmable pixel-mode linear interferometers using multi-plane light conversion</title>
    <updated>2026-08-16T20:15:29Z</updated>
    <link href="https://arxiv.org/abs/2603.15836v2" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2603.15836v2" rel="related" type="application/pdf" title="pdf"/>
    <summary>Programmable linear optical interferometers are a core primitive in optical signal processing, quantum information processing, and photonic computing. Existing photonic-integrated implementations realize arbitrary $M$-mode unitaries using Mach--Zehnder-interferometer meshes whose footprint and accumulated loss scale with $O(M^2)$ optical components. Here we analyze and experimentally demonstrate a programmable architecture for implementing linear optical transformations directly on spatially tiled free-space {\em pixel modes} using multi-plane light conversion (MPLC). In this architecture, $M$ spatial modes arranged on a transverse lattice undergo a unitary transformation and are mapped to $M$ output modes of identical geometry through a sequence of programmable phase masks separated by free-space propagation segments. Numerical simulations show that arbitrary $M$-mode unitaries can be compiled to a desired high fidelity using a number of phase planes that scales approximately linearly with $M$. Using a spatial-light-modulator-based MPLC, we experimentally demonstrate programmable interferometers acting on up to $16$ spatial pixel modes, including tunable beamsplitters, Hadamard unitaries, spatial permutations, and partial unitaries on select subsets of modes. These results establish MPLC-based pixel-mode interferometers as a promising architecture for programmable linear optics with applications in classical and quantum optical interconnects, photonic switching, and quantum information processing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-03-16T19:08:38Z</published>
    <arxiv:comment>21 pages, 22 figures</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Mushkan Sureka</name>
    </author>
    <author>
      <name>Itay Ozer</name>
    </author>
    <author>
      <name>Wenhua He</name>
    </author>
    <author>
      <name>Michael R. Grace</name>
    </author>
    <author>
      <name>Chaohan Cui</name>
    </author>
    <author>
      <name>Saikat Guha</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2603.10667v1</id>
    <title>Low-loss phase-change material based programmable mode converter for photonic computing</title>
    <updated>2026-03-11T11:29:45Z</updated>
    <link href="https://arxiv.org/abs/2603.10667v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2603.10667v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Phase-change materials (PCMs)-based integrated photonic memory offers a viable pathway for the development of neuromorphic computing chip. The sizable optical contrast in the telecom band between amorphous and crystalline phases of PCM, in particular, Ge2Sb2Te5 (GST), is used for multilevel programming. However, the high extinction coefficient k of crystalline GST leads to high optical loss, posing a serious challenge for scaling up the device array for practical use. In this work, we focus on the atomic understanding and application of the so-called low-loss PCM, Sb2Se3, through multiscale simulations. First, we elucidate the bonding origin of the wavelength dependent optical properties of amorphous and crystalline Sb2Se3 via ab initio calculations. Given the suppressed k in the telecom band, we design a programable mode converter (PMC) waveguide device that utilizes only the contrast in refractive index n between amorphous and crystalline Sb2Se3 to encode multiple optical levels per waveguide device. The finite-difference time-domain simulations show that a single PMC device can achieve 5-bit programming precision (32 levels) via direct laser writing, and the photonic tensor core formed by the PMC array could possibly be scaled to 128*128. Finally, a thorough comparison between low-loss PCM and conventional PCM is provided.</summary>
    <category term="cond-mat.mtrl-sci" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-03-11T11:29:45Z</published>
    <arxiv:comment>24 pages, 7 figure, 2 tables</arxiv:comment>
    <arxiv:primary_category term="cond-mat.mtrl-sci"/>
    <author>
      <name>Xueyang Shen</name>
    </author>
    <author>
      <name>Ruixuan Chu</name>
    </author>
    <author>
      <name>Ding Xu</name>
    </author>
    <author>
      <name>Yuan Gao</name>
    </author>
    <author>
      <name>Wen Zhou</name>
    </author>
    <author>
      <name>Wei Zhang</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2602.20910v1</id>
    <title>Novel High-Scalability Architecture for Photonic Deep Learning</title>
    <updated>2026-02-24T13:47:08Z</updated>
    <link href="https://arxiv.org/abs/2602.20910v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2602.20910v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Photonic computing promises ultrafast and energy-efficient artificial intelligence. However, existing photonic neural networks (PNNs) remain functionally shallow and difficult to scale. Here we establish a theory-guided framework showing that power stability and complex-field correlation are the fundamental prerequisites for scalable, coherent PNNs. Building on these macroscopic principles, we introduce the Coherent, Compensated and Cross-connected (C3) unit - an architecture that integrates coherent nonlinearity, active loss compensation and native optical residual connectivity. Implemented on a silicon-on-insulator platform, the C3 unit provides reconfigurable activation functions and dynamic energy stabilization without external amplification. We validate this framework using a width-constrained spiral benchmark, in which the C3 unit substantially improves parameter utilization and power robustness relative to incoherent nonlinearities. In a high-complexity 1,623-class recognition task, our C3-enabled coherent residual network (CoP-ResNet) achieves a top-1 accuracy of 77.92%, whereas non-residual architectures fail to converge. Together, these results offer a physically grounded, theory-guided pathway toward greater optical processing depth, laying the foundation for next-generation, large-scale photonic computing architectures.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-02-24T13:47:08Z</published>
    <arxiv:comment>20 pages, 6 figures</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Yuxin Sun</name>
    </author>
    <author>
      <name>Chun Gao</name>
    </author>
    <author>
      <name>Jin Xie</name>
    </author>
    <author>
      <name>Pan Wang</name>
    </author>
    <author>
      <name>Zejie Yu</name>
    </author>
    <author>
      <name>Yiwei Xie</name>
    </author>
    <author>
      <name>Huan Li</name>
    </author>
    <author>
      <name>Daoxin Dai</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2602.19968v1</id>
    <title>Probabilistic Photonic Computing</title>
    <updated>2026-02-23T15:30:34Z</updated>
    <link href="https://arxiv.org/abs/2602.19968v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2602.19968v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Probabilistic computing excels in approximating combinatorial problems and modelling uncertainty. However, using conventional deterministic hardware for probabilistic models is challenging: (pseudo) random number generation introduces computational overhead and additional data shuffling, which is particularly detrimental for safety-critical applications requiring low latency such as autonomous driving. Therefore, there is a pressing need for innovative probabilistic computing architectures that achieve low latencies with reasonable energy consumption. Physical computing offers a promising solution, as these systems do not rely on an abstract deterministic representation of data but directly encode the information in physical quantities. Therefore, they can be seamlessly integrated with physical entropy sources, enabling inherent probabilistic architectures. Photonic computing is a prominent variant due to the large available bandwidth, several orthogonal degrees of freedom for data encoding and optimal properties for in-memory computing and parallel data transfer. Here, we highlight key developments in physical photonic computing and photonic random number generation. We provide insights into the realization of probabilistic photonic processors and lend our perspective on their impact on AI systems and future challenges.</summary>
    <category term="physics.app-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-02-23T15:30:34Z</published>
    <arxiv:primary_category term="physics.app-ph"/>
    <author>
      <name>Frank Brückerhoff-Plückelmann</name>
    </author>
    <author>
      <name>Anna P. Ovvyan</name>
    </author>
    <author>
      <name>Akhil Varri</name>
    </author>
    <author>
      <name>Hendrik Borras</name>
    </author>
    <author>
      <name>Bernhard Klein</name>
    </author>
    <author>
      <name>C. David Wright</name>
    </author>
    <author>
      <name>Harish Bhaskaran</name>
    </author>
    <author>
      <name>Ghazi Sarwat Syed</name>
    </author>
    <author>
      <name>Abu Sebastian</name>
    </author>
    <author>
      <name>Holger Fröning</name>
    </author>
    <author>
      <name>Wolfram Pernice</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2602.19957v1</id>
    <title>Multidimensional photonic computing</title>
    <updated>2026-02-23T15:24:59Z</updated>
    <link href="https://arxiv.org/abs/2602.19957v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2602.19957v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>The rapidly increasing demands for computational throughput, bandwidth, and memory capacity fueled by breakthroughs in machine learning pose substantial challenges for conventional electronic computing platforms. For digital scaling to keep pace with the accelerating growth of artificial intelligence (AI) models beyond the trajectory of Moores law, computational power has to double roughly every three months. Historically, advancing compute performance relied on spatial scaling to increase the transistor count on a given chip area and, more recently, the development of parallel and multi-core architectures. Exponential scaling on trajectories much steeper than what can be achieved by such conventional strategies, and in line with the demands of AI, can be achieved with computing platforms that process data using multiple, orthogonal dimensions available to photons. Here we elucidate pivotal developments in the realization of multidimensional computing platforms based on photonic systems. Moving to such architectures holds enormous promise for low-latency, high-bandwidth information processing at reduced energy consumption.</summary>
    <category term="physics.app-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-02-23T15:24:59Z</published>
    <arxiv:primary_category term="physics.app-ph"/>
    <author>
      <name>Ivonne Bente</name>
    </author>
    <author>
      <name>Shabnam Taheriniya</name>
    </author>
    <author>
      <name>Francesco Lenzini</name>
    </author>
    <author>
      <name>Frank Brückerhoff-Plückelmann</name>
    </author>
    <author>
      <name>Michael Kues</name>
    </author>
    <author>
      <name>Harish Bhaskaran</name>
    </author>
    <author>
      <name>C David Wright</name>
    </author>
    <author>
      <name>Wolfram Pernice</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2602.19031v2</id>
    <title>SKYLIGHT: A Scalable Hundred-Channel 3D Photonic In-Memory Tensor Core Architecture for Real-time AI Inference</title>
    <updated>2026-03-07T20:37:20Z</updated>
    <link href="https://arxiv.org/abs/2602.19031v2" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2602.19031v2" rel="related" type="application/pdf" title="pdf"/>
    <summary>The growing computational demands of artificial intelligence (AI) are challenging conventional electronics, making photonic computing a promising alternative. However, existing photonic architectures face fundamental scalability and reliability barriers. This paper introduces SKYLIGHT, a scalable 3D photonic in-memory tensor core architecture designed for real-time AI inference. By co-designing its topology, wavelength routing, accumulation, and programming in a 3D stack, SKYLIGHT overcomes key limitations. Its innovations include a low-loss 3D Si/SiN crossbar topology, a thermally robust non-micro-ring resonator (MRR)-based wavelength-division multiplexing (WDM) component, a hierarchical signal accumulation using a multi-port photodetector (PD), and optically programmed non-volatile phase-change material (PCM) weights. Importantly, SKYLIGHT enables in-situ weight updates that support label-free, layer-local learning (e.g., forward-forward local updates) in addition to inference. Using SimPhony for system-level modeling, we show that a single 144 x 256 SKYLIGHT core is feasible within a single reticle and delivers 342.1 TOPS at 23.7 TOPS/W, enabling ResNet-50 inference at 1212 FPS with 27 mJ per image, and achieves 84.17 FPS/W end-to-end (1.61 x higher than an NVIDIA RTX PRO 6000 Blackwell GPU) under the same workload in real-time measurements. System-level evaluations on four representative machine learning tasks, including unsupervised local self-learning, demonstrate SKYLIGHT's robustness to realistic hardware non-idealities (low-bit quantization and signal-proportional analog noise capturing modulation, PCM programming, and readout variations). With noise-aware training, SKYLIGHT maintains high task accuracy, validating its potential as a comprehensive solution for energy-efficient, large-scale photonic AI accelerators.</summary>
    <category term="cs.ET" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.AR" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-02-22T03:50:17Z</published>
    <arxiv:primary_category term="cs.ET"/>
    <author>
      <name>Meng Zhang</name>
    </author>
    <author>
      <name>Ziang Yin</name>
    </author>
    <author>
      <name>Nicholas Gangi</name>
    </author>
    <author>
      <name>Alexander Chen</name>
    </author>
    <author>
      <name>Brett Bamfo</name>
    </author>
    <author>
      <name>Tianle Xu</name>
    </author>
    <author>
      <name>Jiaqi Gu</name>
    </author>
    <author>
      <name>Zhaoran Rena Huang</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2602.18299v1</id>
    <title>Photonic-computing error correction through optical en-/decoder calibrations</title>
    <updated>2026-02-20T15:53:14Z</updated>
    <link href="https://arxiv.org/abs/2602.18299v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2602.18299v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Photonic processors have emerged as an attractive platform for fast and energy-efficient matrix-vector multiplication. However, they are susceptible to error due to their analog nature. Here, we present an error-correction technique that implements a correction offset to the optical en-/decoders of photonic processors. Our proposed method is general-purpose, does not require introducing any additional components to the photonic network, and can address errors stemming from unbalanced losses, 50/50 beamsplitter deviations, digital-to-analog conversion inaccuracies, and any unknown sources. In particular, we show that our method is highly effective in mitigating unbalanced-loss errors, a problem that has not previously been addressed by any error-correction technique. Using this approach, we achieve over 90% error reduction in large triangular meshes, overcoming a key obstacle to highly accurate photonic processors for information processing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-02-20T15:53:14Z</published>
    <arxiv:comment>9 pages and 5 figures</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Adam Carstensen</name>
    </author>
    <author>
      <name>Babak Vosoughi Lahijani</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2602.16927v1</id>
    <title>Free Quantum Computing</title>
    <updated>2026-02-18T22:39:58Z</updated>
    <link href="https://arxiv.org/abs/2602.16927v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2602.16927v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Quantum computing improves substantially on known classical algorithms for various important problems, but the nature of the relationship between quantum and classical computing is not yet fully understood. This relationship can be clarified by free models, that add to classical computing just enough physical principles to represent quantum computing and no more. Here we develop an axiomatisation of quantum computing that replaces the standard continuous postulates with a small number of discrete equations, as well as a free model that replaces the standard linear-algebraic model with a category-theoretical one. The axioms and model are based on reversible classical computing, isolate quantum advantage in the ability to take certain well-behaved square roots, and link to various quantum computing hardware platforms. This approach allows combinatorial optimisation, including brute force computer search, to optimise quantum computations. The free model may be interpreted as a programming language for quantum computers, that has the same expressivity and computational universality as the standard model, but additionally allows automated verification and reasoning.</summary>
    <category term="quant-ph" scheme="http://arxiv.org/schemas/atom"/>
    <category term="math.CT" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-02-18T22:39:58Z</published>
    <arxiv:comment>32 pages</arxiv:comment>
    <arxiv:primary_category term="quant-ph"/>
    <arxiv:journal_ref>Proceedings of the National Academy of Sciences 123(8):e2510881123, 2026</arxiv:journal_ref>
    <author>
      <name>Jacques Carette</name>
    </author>
    <author>
      <name>Chris Heunen</name>
    </author>
    <author>
      <name>Robin Kaarsgaard</name>
    </author>
    <author>
      <name>Neil J. Ross</name>
    </author>
    <author>
      <name>Amr Sabry</name>
    </author>
    <arxiv:doi>10.1073/pnas.2510881123</arxiv:doi>
    <link rel="related" href="https://doi.org/10.1073/pnas.2510881123" title="doi"/>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2602.15762v2</id>
    <title>PRISM: Photonics-Informed Inverse Lithography for Manufacturable Inverse-Designed Photonic Integrated Circuits</title>
    <updated>2026-06-01T22:26:19Z</updated>
    <link href="https://arxiv.org/abs/2602.15762v2" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2602.15762v2" rel="related" type="application/pdf" title="pdf"/>
    <summary>Recent advances in photonic inverse design have demonstrated the ability to automatically synthesize compact, high-performance photonic components that surpass conventional, hand-designed structures, offering a promising path toward scalable and functionality-rich photonic hardware. However, the practical deployment of inverse-designed PICs is bottlenecked by manufacturability: their irregular, subwavelength geometries are highly sensitive to fabrication variations, leading to large performance degradation, low yield, and a persistent gap between simulated optimality and fabricated performance. Unlike electronics, photonics lacks a systematic, flexible mask optimization flow. Fabrication deviations in photonic components cause large optical response drift and compounding error in cascaded circuits, while calibrating fabrication models remains costly and expertise-heavy, often requiring repeated fabrication cycles that are inaccessible to most designers. To bridge this gap, we introduce PRISM, a photonics-informed inverse lithography workflow that makes photonic mask optimization data-efficient, reliable, and optics-informed. PRISM (i) synthesizes compact, informative calibration patterns to minimize required fabrication data, (ii) trains a physics-grounded differentiable fabrication model, enabling gradient-based optimization, and (iii) performs photonics-informed inverse mask optimization that prioritizes performance-critical features beyond geometry matching. Across multiple inverse-designed components with both electron-beam lithography and deep ultra-violet photolithography processes, PRISM significantly boosts post-fabrication performance and yield while reducing calibration area and turnaround time, enabling and democratizing manufacturable and high-yield inverse-designed photonic hardware at scale.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <category term="cs.ET" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-02-17T17:48:44Z</published>
    <arxiv:comment>26 pages. Accepted to ACM TODAES Special Issue on Co-Design and Design Automation for Optical/Photonic Computing Systems, 2026</arxiv:comment>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Hongjian Zhou</name>
    </author>
    <author>
      <name>Haoyu Yang</name>
    </author>
    <author>
      <name>Nicholas Gangi</name>
    </author>
    <author>
      <name>Tianle Xu</name>
    </author>
    <author>
      <name>Rena Huang</name>
    </author>
    <author>
      <name>Jiaqi Gu</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2602.12938v1</id>
    <title>All-Optically Controlled Memristive Reservoir Computing Capable of Bipolar and Parallel Coding</title>
    <updated>2026-02-13T13:50:30Z</updated>
    <link href="https://arxiv.org/abs/2602.12938v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2602.12938v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Physical reservoir computing (RC) utilizes the intrinsic dynamical evolution of physical systems for efficient data processing. Emerging optoelectronic RC platforms,such as light-driven memristors, merge the benefits of electronic and photonic computation. However, conventional designs are often limited by the unipolar photoresponse of optoelectronic devices, which restricts reservoir state diversity and reduces computational accuracy. To overcome these limitations, we introduce an all-optically controlled RC system employing an oxide memristor array that demonstrates exceptional uniformity and stability. The memristive devices exhibit wavelength-dependent bipolar photoresponse, originating from light-induced dynamic evolution of oxygen vacancies. Tuning the power density and irradiation mode of dual-wavelength light pulses enables dynamic control of photocurrent relaxation and nonlinearity. By leveraging these unique device properties, we develop bipolar and parallel coding strategies to significantly enrich reservoir dynamics and enhance nonlinear mapping capability. In word recognition and time-series prediction tasks, the bipolar coding demonstrates markedly improved accuracy compared to unipolar coding. The parallel coding supports multi-source signal fusion within a single reservoir, maintaining high computational accuracy while significantly reducing hardware consumption. This work provides a high-performance approach to physical RC, paving the way for intelligent edge computing.</summary>
    <category term="physics.app-ph" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-02-13T13:50:30Z</published>
    <arxiv:comment>33 pages, 11 figures</arxiv:comment>
    <arxiv:primary_category term="physics.app-ph"/>
    <author>
      <name>Lingxiang Hu</name>
    </author>
    <author>
      <name>Dian Jiao</name>
    </author>
    <author>
      <name>Kexuan Wang</name>
    </author>
    <author>
      <name>Peihong Cheng</name>
    </author>
    <author>
      <name>Jingrui Wang</name>
    </author>
    <author>
      <name>Li Zhang</name>
    </author>
    <author>
      <name>Athanasios V. Vasilakos</name>
    </author>
    <author>
      <name>Yang Chai</name>
    </author>
    <author>
      <name>Zhizhen Ye</name>
    </author>
    <author>
      <name>Fei Zhuge</name>
    </author>
  </entry>
  <entry>
    <id>http://arxiv.org/abs/2602.11697v1</id>
    <title>Hybridized-band parametric oscillations in coupled Kerr microresonators</title>
    <updated>2026-02-12T08:23:01Z</updated>
    <link href="https://arxiv.org/abs/2602.11697v1" rel="alternate" type="text/html"/>
    <link href="https://arxiv.org/pdf/2602.11697v1" rel="related" type="application/pdf" title="pdf"/>
    <summary>Coupled resonators form band-like optical states that support rich nonlinearities beyond what is possible in single resonators. In these systems, four-wave mixing mediates interband coupling, displaying multimode dynamics that span both spatial and spectral degrees of freedom. In this study, we propose a framework describing the onset and control of hybridized optical parametric oscillation in three coupled silicon nitride microring resonators. In a symmetric configuration, we observe the emergence of diverse phase-matching pathways defined by the dispersive band structure. We develop an analytical model that captures the parametric gain of these interband processes and derive closed-form expressions for the dominant gain maxima; the analytical framework itself readily extends to more complex coupled networks. We further report an asymmetric design that co-engineers mode overlap and dispersion to operate on a compact 7-GHz spacing, free from mode competition. Our findings establish design principles for engineering nonlinear dynamics in coupled-resonator platforms, with implications for coherent photonic computing and quantum information processing.</summary>
    <category term="physics.optics" scheme="http://arxiv.org/schemas/atom"/>
    <published>2026-02-12T08:23:01Z</published>
    <arxiv:primary_category term="physics.optics"/>
    <author>
      <name>Luca O. Trinchão</name>
    </author>
    <author>
      <name>Luiz Peres</name>
    </author>
    <author>
      <name>Eduardo S. Gonçalves</name>
    </author>
    <author>
      <name>Miguel Nienstedt</name>
    </author>
    <author>
      <name>Laís Fujii dos Santos</name>
    </author>
    <author>
      <name>Paulo F. Jarschel</name>
    </author>
    <author>
      <name>Thiago P. Mayer Alegre</name>
    </author>
    <author>
      <name>Nathalia B. Tomazio</name>
    </author>
    <author>
      <name>Gustavo S. Wiederhecker</name>
    </author>
  </entry>
</feed>
