Zhao Guanghui, Lin Jintian, Gao Renhong, Hou Qifeng, Guan Jianglin, Li Chuntao, Zheng Xinzhi, Li Minghui, Luo Xiaochao, Qiu Yingnuo, Qiao Lingling, Wang Min, Cheng Ya
Opt Lett. 2025 Jul 1;50(13):4310-4313. doi: 10.1364/OL.565825.
Periodically poled lithium niobate on insulator (PPLNOI) ridge waveguides are essential photonic components for both classical and quantum information processing. However, dry etching of PPLNOI waveguides frequently generates rough sidewalls and variations in the etching rates of oppositely poled lithium niobate ferroelectric domains, leading to relatively high propagation losses (0.25-1 dB/cm), which significantly limits net conversion efficiency and hinders scalable photonic integration. In this work, a low-loss PPLNOI ridge waveguide with a length of 7 mm was fabricated using ultra-smooth sidewalls through photolithography-assisted chemo-mechanical etching followed by high-voltage pulse poling with low cost. The average surface roughness was measured to be only 0.27 nm, resulting in a record-low propagation loss of 0.11 dB/cm in PPLNOI waveguides. Highly efficient second harmonic generation was demonstrated with a normalized efficiency of 1643% W·cm without temperature tuning, corresponding to a conversion efficiency of 805%/W, which is close to the best conversion efficiency reported in nanophotonic PPLNOI waveguide fabricated by expensive electron-beam lithography followed by dry etching, and the absolute conversion efficiency reached 15.7% at a pump level of 21.6 mW. The normalized efficiency can be even improved to 1742% W·cm at the optimal temperature of 59C.
周期性极化绝缘体上铌酸锂(PPLNOI)脊形波导是经典和量子信息处理中必不可少的光子组件。然而,PPLNOI波导的干法蚀刻经常会产生粗糙的侧壁,并且相反极化的铌酸锂铁电畴的蚀刻速率会发生变化,从而导致相对较高的传播损耗(0.25 - 1 dB/cm),这显著限制了净转换效率并阻碍了可扩展的光子集成。在这项工作中,通过光刻辅助化学机械蚀刻制造了具有超光滑侧壁的低损耗PPLNOI脊形波导,其长度为7 mm,随后采用低成本的高压脉冲极化。测量得到的平均表面粗糙度仅为0.27 nm,在PPLNOI波导中实现了创纪录的低传播损耗0.11 dB/cm。在无需温度调谐的情况下,实现了高效的二次谐波产生,归一化效率为1643% W·cm,对应于805%/W的转换效率,这接近通过昂贵的电子束光刻和干法蚀刻制造的纳米光子PPLNOI波导中报道的最佳转换效率,并且在泵浦功率为21.6 mW时绝对转换效率达到15.7%。在59°C的最佳温度下,归一化效率甚至可以提高到1742% W·cm。