Fig. 3 Mechanism and result of the super-resolution RLP.

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Presentation transcript:

Fig. 3 Mechanism and result of the super-resolution RLP. Mechanism and result of the super-resolution RLP. (A) Mechanism of the formation of a focal spot by overlapping the excitation beam and the periodical resonator array. A Gaussian excitation beam with low power (i) is enhanced and modified by the periodical resonators supporting highly confined localized resonances (ii), producing an effective photothermal heating area smaller than a diffraction-limited spot (iii). Scale bar, 200 nm. The original laser power for super-resolution printing should not exceed the threshold for melting an unstructured Ge thin film, whereas the locally enhanced energy density should overcome the threshold to initialize photothermal reshaping processes. (B) SEM image shows the RLP within a single unit cell, addressing the morphology change of the centered particle. Scale bar, 200 nm. (C) RLP images with a resolution of 127,000 DPI. The samples are with T = 35 nm and R = 70 nm (left), 80 nm (middle), and 90 nm (right), respectively. Scale bars, 10 μm. (D) SEM image of an RLP image in (C), which shows details of the structure and the corresponding electron scattering changes induced by laser printing. Scale bar, 10 μm. (E) SEM image of an enlarged region of the image in (D), showing the remarkable detail and morphology change on a single–unit cell level. These modified unit cells exhibit different colors in the optical image because of an RLP-induced variation in nanodisk sizes and the ablation of the disks. Scale bar, 200 nm. Xiaolong Zhu et al. Sci Adv 2017;3:e1602487 Copyright © 2017, The Authors