Abstract

Why can we not see nanoscale objects under a light microscope? The textbook answers are that their relative signals are weak and their separation is smaller than Abbe’s resolution limit. Thus, significant effort has gone into developing ultraviolet imaging, oil and solid immersion objectives, nonlinear methods, fluorescence dyes, evanescent wave tailoring, and point-spread function engineering. In this work, we introduce a new optical sensing framework based on the concepts of electromagnetic canyons and non-resonance amplification, to directly view on a widefield microscope λ/31-scale (25-nm radius) objects in the near-field region of nanowire-based sensors across a 726-μm × 582-μm field of view. Our work provides a simple but highly efficient framework that can transform conventional diffraction-limited optical microscopes for nanoscale visualization. Given the ubiquity of microscopy and importance of visualizing viruses, molecules, nanoparticles, semiconductor defects, and other nanoscale objects, we believe our proposed framework will impact many science and engineering fields.

Highlights

  • The weak scattering signal, can be overwhelmed by the background signal that is induced by the scattering from surrounding patterns/ substrates as well as by fluctuations induced by system errors and the instability of the instruments in a conventional microscope[10]

  • Our proposal overcomes the aforementioned limitations of conventional methods by artificially creating an electromagnetic canyon (EC; the region where background electromagnetic field is null), such that the far-field scattering of a nanoscale object amplified by a non-resonance nanostructure ensemble can be directly imaged in a conventional optical microscope

  • The generation of the EC is built upon the scalar theory that two point sources coherently emitting 180° out of phase can be resolved in a microscope intensity image regardless of the gap size[27]

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Summary

Introduction

EC resoNnaonnc- e S Position Energy (eV). Metallic particles expansion analysis combined with coupled mode perturbation theory shows that the electric field ESP(r) around the symmetry plane (SP) (see the transparent plane marked with “SP” in Fig. 2a and b) can be represented by (see Supplementary Note 1)[28,29,30,31]

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