Acta Optica Sinica, Volume. 45, Issue 14, 1420003(2025)

Photonic Computing Based on Microring Resonator (Invited)

Chaoran Huang*, Shaojie Liu, Benshan Wang, Dongliang Wang, Yikun Nie, and Tengji Xu
Author Affiliations
  • Department of Electronic Engineering, The Chinese University of Hong Kong, Hong Kong 999077, China
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    Figures & Tables(16)
    Artificial intelligent computing. (a) Linear and nonlinear computing; (b) deep neural network; (c) reservoir computing
    MRR. (a) All-pass MRR. (b) add-drop MRR
    Schematic of WDM-based MVM system. (a) Basic MVM[50]; (b) schematic diagram of MRR weight bank[50]; (c) schematic diagram of single-end detection MRR array[51]; (d) schematic diagram of crossbar MRR array[52]; (e) schematic diagram of PCM array[6]
    MRR MVM weight bank for linear signal processing. (a) Pulse shaping using MRR array[53]; (b) linear binary MVM using MRR array[54]; (c) schematic diagram of WDM scalable “broadcast and weight” architecture[50]; (d) arbitrary continuous positive/negative MVM using MRR weight bank[55]; (e) optoelectronic recurrent neural network using MRR weight bank[56]; (f) all optical neuromorphic processing using PCM and MRRs[57]; (g) ultra-high parallelism MVM using the PCM array[6]
    Novel optical computing architecture based on the MRRs. (a)(b) Simultaneously achieving neural network forward propagation and back propagation using MRR[52,58]; (c) high order tensor convolution processing using MRR[44]; (d) high parallelism convolution using MRR and optical frequency comb[45]; (e) MRR array based on MDM and WDM[59]; (f) high-dimensional lightwave and microwave multidomain multiplexing integrated photonic tensor core[60]; (g) high endurance MRR array based on non-reciprocal magneto-optics with ultra-high endurance[61]; (h) electrically programmable and non-volatile MRR array based on phase-change materials[62]
    Microring architecture and its all-optical nonlinear response. (a) Microring architecture and its key parameters; (b) time scale of various nonlinear effects in microrings; (c) resonant response of microrings and the changes in the red and blue shifts of their resonant wavelengths; (d) hysteresis curves of microring output power and input power; (e) temporal variations of output power, intracavity energy, temperature changes, and free carrier concentration in microrings
    All-optical reconfigurable nonlinear activation functions based on MRR. (a)(b) All-optical reconfigurable nonlinear activation functions based on silicon MRR-assisted MZI[72]; (c)(d) all-optical reconfigurable nonlinear activation functions based on silicon nitride MRR with PCM[57]; (e)(f) all-optical reconfigurable nonlinear activation functions based on silicon MRR with PCM[73]; (g)(h) all-optical reconfigurable nonlinear activation functions based on Ge/Si hybrid MRR[74]
    All-optical MRR spiking neurons. (a) Structure and basic properties of biological spiking neurons; (b1)‒(b4) silicon MRR spiking neuron[70]; (c1)‒(c3) silicon MRR spiking neuron with suppressed refractory period[76]; (d1)‒(d4) hybrid graphene-on-silicon MRR spiking neuron[77]
    Major advances in OEO photonic neurons based on microring resonators. (a) First integrated OEO neuron based on silicon microring modulator[81]; (b) integrated OEO neuron based on microring modulator and on-chip trans-impedance[7]; (c) wire-bonded OEO neuron based on microring modulator and off-chip trans-impedance amplifier chip[9]; (d) integrated OEO neuron based on microring modulator in a programmable configuration[13]
    Optical computing system based on MRR for AI. (a) DONN based on MRR weight bank and OEO MRR neuron[7]; (b) DONN based on on-chip optical attenuators and OEO MRR neuron[9]; (c) DONN based on MZI-mesh and OEO MRR neuron[13]; (d) space-division-multiplexing optical reservoir computing based on all-optical nonlinearity of MRR[83]; (e) time-division-multiplexing optical reservoir computing without feedback loop based on all-optical nonlinearity of MRR[84]; (f) time-division-multiplexing optical reservoir computing with feedback loop based on all-optical nonlinearity of MRR[85]
    MRR weight control and high-precision computing. (a) Feedback control based on N-doped MRR[86]; (b) 9 bit weight precision realized by dithering control[88]; (c) self-calibrating weight with dual-wavelength synchronization[89]; (d) 11.3 bit weight precision of single MRR based on all-analog circuits[91]; (e) over 9 bit weight precision realized by calibration-free Chil-in-the-loop optimization[90]; (f) digital-analog hybrid computing achieves 16 bit computing precision[92]
    Optical computing system robust optimization. (a) Noise-aware training enables system operates stably with system low precision control[93]; (b) noise-aware training improves system robustness against high-speed system noise[94]; (c) noise-aware training improves generative model’s robustness against noise[95]; (d) hardware-aware training achieves MRR stable operation without TEC by alleviating MRR’s component stability[96]; (e) hardware-aware training significantly improves model's robustness by simultaneously alleviating component stability and system stability[97]
    Applications of MRR in photonic computing. (a) MRR array for solving NP-complete problems[105]; (b) MRR array for solving partial differential equations (PDEs)[106]; (c) MRR array for compensating nonlinear effects in optical fibers[7]; (d) MRR array for solving dynamic radio-frequency interference problems[107]; (e) MRR array for compensating dispersion effects in optical fibers[108]; (f) MRR array for analog spatiotemporal feature extraction[109]; (g) MRR array for end-to-end image processing[110]
    • Table 1. Definition and values of relevant parameters of the MRR[68,70]

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      Table 1. Definition and values of relevant parameters of the MRR[68,70]

      ParameterDescriptionValue
      dnSi /dTThermo-optic coefficient of silicon1.86×10-4 K-1
      dnSi /dNFree carrier coefficient of silicon-1.73×10-27 m3
      dnSi /da2Kerr coefficient of silicon5.18×10-7 J-1
      σSiFree carrier absorption cross section1×10-21 m2
      ρSiDensity of bulk silicon2.33 g·cm-3
      βSiTwo-photon absorption coefficient of silicon8.4×10-12 m·W-1
      cp,SiThermal capacity of silicon0.7 J·g-1·K-1
      ngGroup index of silicon waveguide4.496
      ΓFCAFree carrier confinement factor0.996
      VFCAFree carrier effective volume5.862 µm3
      ΓTPATwo-photon absorption confinement factor0.9836
      VTPATwo-photon absorption effective volume6.585 µm3
      ΓthThermal confinement factor0.8956
      VthThermal effective volume10.39 µm3
      γabs,linLinear absorption loss constant0.976 ns-1
      γradRadiation loss constant49.7 ns-1
      τthThermal lifetime102 ns
      τfcFree carrier lifetime4.5 ns
    • Table 2. Implementation schemes of MRR-based all-optical reconfigurable nonlinear activation functions

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      Table 2. Implementation schemes of MRR-based all-optical reconfigurable nonlinear activation functions

      Ref.Experimental schemeMain physical mechanismsDemonstrated activation functionsReconfiguration methodReconfiguration complexityEnergy consumption
      [72]Silicon MRR-assisted MZIFCDClamped ReLU, Radial Basis, Sigmoid, SoftplusPhase shifterLowHigh
      [57]Silicon nitride MRR with PCMCrystalline and amorphous states of PCMReLUChange the operation wavelengthHighLow
      [73]Silicon MRR with PCMThermo-optic and free-carrier-related effectsRadial Basis, ReLU, Softplus, ELUChange the crystallization fraction of PCMHighLow
      [74]Ge/Si hybrid MRRThermo-optic effectRadial Basis, ReLU, ELUChange the operation wavelengthHighLow
    • Table 3. Implementation schemes of MRR-based all-optical spiking neurons

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      Table 3. Implementation schemes of MRR-based all-optical spiking neurons

      Ref.Spiking neuronMain physical mechanismsExcited pulse time scaleRefractory periodOperation speed
      [70]Silicon MRRThermo-optic effect and FCDNanosecond60 ns16 MHz
      [76]Silicon MRRThermo-optic effect and FCDNanosecondBe suppressedSub-GHz
      [77]Graphene-on-silicon MRRFCD and the saturable absorption in graphenePicosecondNot mentioned~GHz
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    Chaoran Huang, Shaojie Liu, Benshan Wang, Dongliang Wang, Yikun Nie, Tengji Xu. Photonic Computing Based on Microring Resonator (Invited)[J]. Acta Optica Sinica, 2025, 45(14): 1420003

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    Paper Information

    Category: Optics in Computing

    Received: Apr. 15, 2025

    Accepted: Jun. 30, 2025

    Published Online: Jul. 21, 2025

    The Author Email: Chaoran Huang (crhuang@ee.cuhk.edu.hk)

    DOI:10.3788/AOS250932

    CSTR:32393.14.AOS250932

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