Jeong Tae-In, Oh Dong Kyo, Kim San, Park Jongkyoon, Kim Yeseul, Mun Jungho, Kim Kyujung, Chew Soo Hoon, Rho Junsuk, Kim Seungchul
Department of Cogno-Mechatronics Engineering, College of Nanoscience and Nanotechnology, Pusan National University, Busan 46241, Republic of Korea.
Department of Mechanical Engineering, Pohang University of Science and Technology (POSTECH), Pohang 37673, Republic of Korea.
Nanophotonics. 2022 Oct 24;12(3):619-629. doi: 10.1515/nanoph-2022-0365. eCollection 2023 Feb.
Plasmonic nanoantennas have been extensively explored to boost nonlinear optical processes due to their capabilities to confine optical fields on the nanoscale. In harmonic generation, nanoantenna array architectures are often employed to increase the number of emitters in order to efficiently enhance the harmonic emission. A small laser focus spot on the nanoantenna array maximizes the harmonic yield since it scales nonlinearly with the incident laser intensity. However, the nonlinear yield of the nanoantennas lying at the boundary of a focused beam may exhibit significant deviations in comparison to those at the center of the beam due to the Gaussian intensity distribution of the beam. This spatial beam inhomogeneity can cause power instability of the emitted harmonics when the lateral beam position is not stable which we observed in plasmon-enhanced third-harmonic generation (THG). Hence, we propose a method for deterministically designing the density of a nanoantenna array to decrease the instability of the beam position-dependent THG yield. This method is based on reducing the ratio between the number of ambiguous nanoantennas located at the beam boundary and the total number of nanoantennas within the beam diameter to increase the plasmon-enhanced THG stability, which we term as the ratio of ambiguity (). We find that the coefficient of variation of the measured plasmonic THG yield enhancement decreases with the . Thus, our method is beneficial for designing reliable sensors or nonlinear optical devices consisting of nanoantenna arrays for enhancing output signals.
由于等离激元纳米天线能够将光场限制在纳米尺度,因此已被广泛用于增强非线性光学过程。在谐波产生中,经常采用纳米天线阵列结构来增加发射器的数量,以有效增强谐波发射。纳米天线阵列上的小激光聚焦光斑可使谐波产率最大化,因为它与入射激光强度呈非线性比例关系。然而,由于光束的高斯强度分布,位于聚焦光束边界的纳米天线的非线性产率与光束中心的纳米天线相比可能会出现显著偏差。当横向光束位置不稳定时,这种空间光束不均匀性会导致发射谐波的功率不稳定,这一点我们在等离激元增强三次谐波产生(THG)中已经观察到。因此,我们提出了一种确定性设计纳米天线阵列密度的方法,以降低与光束位置相关的THG产率的不稳定性。该方法基于降低位于光束边界的模糊纳米天线数量与光束直径内纳米天线总数之间的比率,以提高等离激元增强THG的稳定性,我们将其称为模糊比率()。我们发现,测量得到的等离激元THG产率增强的变异系数随而降低。因此,我们的方法有利于设计由纳米天线阵列组成的可靠传感器或非线性光学器件,以增强输出信号。