Photonics Research, Volume. 13, Issue 7, 1832(2025)

Scalable and rapid programmable photonic integrated circuits empowered by Ising-model intelligent computation On the Cover

Menghan Yang1,2,3、†, Tiejun Wang4、†, Yuxin Liang5、†, Ye Jin1,2,3, Wei Zhang4, Xiangyan Meng1,2,3, Ang Li1,2,3, Guojie Zhang1,6, Wei Li1,2,3, Nuannuan Shi1,2,3,7、*, Ninghua Zhu1, and Ming Li1,2,3,8、*
Author Affiliations
  • 1State Key Laboratory of Optoelectronic Materials and Devices, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
  • 2College of Materials Science and Opto-Electronic Technology, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3School of Electronic, Electrical and Communication Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 4State Key Laboratory of Information Photonics and Optical Communications and School of Science, Beijing University of Posts and Telecommunications, Beijing 100876, China
  • 5United Microelectronics Center Co., Ltd., Chongqing 401332, China
  • 6China Academy of Space Technology (Xi’an), Xi’an 710100, China
  • 7e-mail: nnshi@semi.ac.cn
  • 8e-mail: ml@semi.ac.cn
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    Figures & Tables(10)
    Programmable PICs and the equivalent Ising model. (a) The structure of programmable PICs consists of a cascading arrangement of hexagonal structures, with each MZI as a programmable basic unit. The MZI is designed with a phase shifter in one arm, enabling precise control over the optical power. (b) The correspondence states between the MZI and the binary decision variable. The MZI’s cross state at θ=0 corresponds to the node state “0,” whereas the MZI’s bar state at θ=π is equated with the node state “1.” (c) The equivalent Ising network model and Ising-model intelligent computation process. A complete Ising matrix is formulated by incorporating the constraints matrix into the Ising model and then finding the optimal solution via an Ising machine to enable dynamic control over the PICs. MZI, Mach–Zehnder interferometer; PS, phase shifter.
    Characteristics of programmable PICs. (a) Microscope image of programmable PICs. (b) Packaged programmable PICs. (c) Test results of five cascaded DCs. (d) Transmission performance of an MZI unit. DC, directional coupler.
    Process of Ising-model intelligent computation. (a) Flow chart of the Ising model-based intelligent computation; (b) minimum Ising energy list for each of the 25 times of iterative calculations. (c) Ising energy evolution process over time of the 7th calculation and the result for four-input four-output intelligent computation. (d) Test results of the stochastic path analog signal processing. (e) Test results of selective path analog signal processing after reconfiguration.
    The programmable PICs in analog signal processing for wavelength routing. (a) Schematic diagram. LD, laser diode; PC, polarization controller; DRV, driver; AM, amplitude modulator; EDFA, erbium-doped optical fiber amplifier; PD, photodetector. (b) The results of Ising-model-based intelligent computation for wavelength routing path planning. (c) Output spectrum with wavelengths at 1535 nm for Path 1, 1540 nm for Path 2, 1545 nm for Path 3, and 1550 nm for Path 4. (d1)–(d4) Eye diagram of 10 Gbaud NRZ signals. (d5)–(d8) Eye diagram of 10 Gbaud NRZ signals after passing through the programmable PICs. (e1)–(e4) Eye diagram of 10 Gbaud PAM-4 signals. (e5)–(e8) Eye diagram of 10 Gbaud PAM-4 signals after passing through the programmable PICs.
    ONN recognition with the programmable PIC-based linear matrix as the convolutional kernel. (a) Schematic diagram of an ONN incorporating programmable PICs for the convolution layer and FPGA for the fully connected layer. (b) The path-planning results of Ising-model-based intelligent computation using the linear matrix X. (c) The comparison between the experimental results and the theoretical values. (d) ONN recognition results for handwritten digits with the programmable PICs as the convolutional kernel.
    Schematic diagram of the hexagonal arrangement of the programmable PIC scale expansion.
    Schematic diagram of the system amplitude representing Ising spins.
    Sensitivity analysis of programmable PICs to temperature variations and fabrication errors. (a) Schematic diagram of the multi-physics simulation model setup (not to scale). (b) Temperature distribution around the waveguide as a function of applied voltage. (c) Phase shift of the waveguide as a function of thermal tuning voltage. (d) Splitting ratio variation caused by ±100 nm changes in the waveguide width of the DC. (e) Splitting ratio variation caused by ±100 nm changes in the gap of the DC coupling region.
    The correspondence between the unit structure MZI and the Ising equivalent model after multi-qubit quantization.
    • Table 1. Performance Comparison of Our Solution Algorithm

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      Table 1. Performance Comparison of Our Solution Algorithm

      AlgorithmMZIsSolution ScaleProcessorSingle Calculation TimeTotal Calculation Time
      GA [34]401×1/0.07 s7.44 s
      Dijkstra [36]a426×64-core CPU at 2.80 GHz0.78 s78.85 s
      Light-processing functions [38]b551×316-core Intel Xeon E7-4850 CPU at 2.1 GHz65.40 s/
      Ising (this work)464×46-core Intel Core i7-9750H CPU (12 threads at 2.6–4.5 GHz)1.43 s71.50 s
      MPIM [47]1.00×104  s7.00×104  s
      Expected from this work200056×56NVIDIA A100 GPU7.20×104  s3.60×106  sc
      MPIM [47]6.00×104  s3.00×102  s
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    Menghan Yang, Tiejun Wang, Yuxin Liang, Ye Jin, Wei Zhang, Xiangyan Meng, Ang Li, Guojie Zhang, Wei Li, Nuannuan Shi, Ninghua Zhu, Ming Li, "Scalable and rapid programmable photonic integrated circuits empowered by Ising-model intelligent computation," Photonics Res. 13, 1832 (2025)

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    Paper Information

    Category: Silicon Photonics

    Received: Dec. 27, 2024

    Accepted: Apr. 14, 2025

    Published Online: Jun. 18, 2025

    The Author Email: Nuannuan Shi (nnshi@semi.ac.cn), Ming Li (ml@semi.ac.cn)

    DOI:10.1364/PRJ.554170

    CSTR:32188.14.PRJ.554170

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