Boris Kalinic, Stefano Vezzoli, Neil Patel, Cynthia Vidal, Benjamin Tilmann, Stefan A. Maier, Riccardo Sapienza, Giovanni Mattei
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引用次数: 0
摘要
我们提出了一种双谐振纳米腔,用于在可见光范围内产生二次谐波(SHG),由590nm的晶体磷化镓(c-GaP)层,金镜和二氧化硅间隔层组成,以实现泵浦和谐波共振的最佳重叠。实验结果表明,该晶体的转换效率跨越4个数量级,在λSHG = 600 nm处最大η η max = 0.014%,与性能最好的半导体超表面相当,比400 μm GaP晶体高出一个数量级以上。利用非线性散射理论,我们解释了光谱响应,并通过入射角或间隔层厚度的调整证明了波长的可调性。我们将这一结果扩展到具有超薄金顶层的封闭腔设计中,我们预测当c-GaP层的厚度接近相干长度时,可以实现高达η→max ~ 0.4%的效率。该设计可扩展到具有更高q因子的平面纳米腔,并用于增强超表面的性能,将非线性转换效率推向实际应用。
Doubly Resonant c-GaP Nanocavity for Second Harmonic Generation
We present a doubly resonant nanocavity for second harmonic generation (SHG) in the visible range, consisting of a 590 nm crystalline gallium phosphide (c-GaP) layer, a gold mirror, and a silica spacer to achieve optimal overlap of pump and harmonic resonances. Experimental results show a conversion efficiency spanning 4 orders of magnitude, with a maximum η̃max = 0.014% at λSHG = 600 nm, comparable to best-performing semiconductor metasurfaces, and surpassing a bulk 400 μm GaP crystal by over an order of magnitude. Using nonlinear scattering theory, we explain the spectral response and demonstrate wavelength tunability via angle of incidence or spacer thickness adjustments. We extend this result to a closed-cavity design with an ultrathin gold top layer which we predict can achieve efficiencies up to η̃max ∼ 0.4% when the thickness of the c-GaP layer approaches the coherence length. This design can be scaled up to planar nanocavities with higher Q-factor and used to enhance the performance of metasurfaces, advancing nonlinear conversion efficiency toward practical applications.
期刊介绍:
Published as soon as accepted and summarized in monthly issues, ACS Photonics will publish Research Articles, Letters, Perspectives, and Reviews, to encompass the full scope of published research in this field.