• 摘要: 片上光学相控阵 (Optical phased array, OPA)因其集成化、高稳定性和高指向精度,在高速光通信中应用前景广阔。然而,片上多孔径天线间的波导光程差异会引入相对时延与相位差,严重劣化系统性能。时延导致接收信号脉冲展宽,引发码间串扰;相位差则降低远场桶中功率,削弱接收信噪比。二者共同作用将显著提升系统误码率。为量化其影响,本文基于OptiSystem与MATLAB构建了片上OPA多孔径协同通信仿真模型,系统分析了时延与相位差的容限。仿真结果表明:对于10 Gbps NRZ-OOK调制的两孔径系统,时延容限为70 ps,相位差容限为0.455π;对于六孔径系统,时延统计分布容限为80 ps。在此范围内,系统误码率可维持在10−9以下。本研究为高性能片上OPA通信系统的参数优化与同步控制设计提供了关键依据,并通过实验验证了仿真分析的主要结论,协同通信技术在抑制孔径间时间延迟和活塞相位差的条件下,有效改善系统通信性能。

       

      Abstract:
      Objective On-chip optical phased arrays (OPAs) provide compact structure, high integration, and precise beam steering capability. These features support their application in free-space optical communication (FSOC) systems. Single-aperture OPAs suffer from limited emission power and relatively large beam divergence. Multi-aperture cooperative transmission improves emission power and far-field directivity. Optical path differences exist between apertures in such structures. Relative time delay and piston phase difference are generated between emitted signals. Time delay causes pulse broadening at the receiver and induces intersymbol interference (ISI). Piston phase difference reduces far-field power concentration, defined by power in the bucket (PIB), and leads to a decrease in received signal-to-noise ratio (SNR). Communication performance is degraded by the combined effects of these two factors. Existing studies focus on coherent beam combining, while communication performance analysis remains insufficient. Quantitative evaluation of time delay and piston phase difference effects is required for system design.
      Methods A joint simulation framework was established using OptiSystem and MATLAB. A cooperative communication system based on on-chip multi-aperture OPAs was constructed. A 10 Gbps NRZ-OOK modulation format was used. The carrier wavelength was 1550 nm. The receiver employed an intensity modulation and direct detection scheme. A photodetector and a low-pass filter with 10 GHz bandwidth were adopted. Controllable time delay was introduced in different aperture branches. Two-aperture and six-aperture configurations were analyzed. Bit error rate (BER), eye diagrams, and signal waveforms were used to evaluate communication performance. A near-field complex amplitude model was built in MATLAB for piston phase difference analysis. Far-field intensity distribution was obtained using Fourier transform. Power in the bucket (PIB) was used to characterize far-field energy concentration. Variations in PIB were mapped to received SNR. These SNR values were applied in the OptiSystem model to obtain BER results.
      Combined effects of time delay and piston phase difference were evaluated by introducing both impairments simultaneously. An experimental system with two apertures was constructed. Relative time delay was adjusted using an optical fiber delay line. A lithium niobate phase modulator was controlled by a stochastic parallel gradient descent algorithm to achieve co-phasing control.
      Results and Discussions Time delay shows a clear impact on communication performance in the two-aperture configuration. When the delay is below approximately 60 ps, ISI remains weak and BER stays at a low level. BER exceeds 10−9 when the delay reaches approximately 70 ps. Communication requirements are no longer satisfied at this point. Time delay in the six-aperture system follows a random distribution. BER remains below 10−9 when the delay range does not exceed 80 ps. BER increases significantly when the range exceeds 80 ps. System stability is degraded.Piston phase difference reduces normalized far-field PIB from 0.74 to approximately 0.31. Received signal power decreases, SNR decreases accordingly. BER increases with increasing phase difference. Under zero time delay, the phase difference tolerance is approximately 0.455 π for BER below 10−9. Combined effects of time delay and piston phase difference further degrade system performance. Tolerance ranges are reduced. Under a time delay of 50 ps, phase difference tolerance decreases to approximately 0.262 π. Time delay induces ISI and enhances performance degradation at a given phase difference. Phase difference reduces SNR and lowers tolerance to time delay. These effects jointly compress the system performance margin.
      Experimental results are close to simulation results and show consistent variation trends. Under co-phasing control, BER starts to increase at a time delay of 60 ps. BER exceeds 10−9 when the delay is greater than 75 ps. Independent compensation methods were also evaluated. Co-phasing control alone or time-delay compensation alone improves performance only partially. Simultaneous application of both methods maintains error-free performance.
      Conclusions Time delay and piston phase difference affect NRZ-OOK communication performance in on-chip multi-aperture OPA systems. Time delay tolerance is approximately 70 ps in the two-aperture configuration. Phase difference tolerance is approximately 0.455 π under zero delay. Delay range should be controlled within 80 ps in the six-aperture configuration to maintain BER below 10−9. Combined impairments reduce system tolerance and compress performance margin. Co-phasing control and time-delay compensation are both required for stable communication.Simulation results are supported by experimental observations. These results provide quantitative guidance for parameter design and synchronization control in on-chip multi-aperture OPA communication systems.