Abstract

An electron bunch passing through a periodic metal grating can emit Smith-Purcell radiation (SPR). Recently, it has been found that SPR can be locked and enhanced at some emission wavelength and angle by excitation of surface plasmon (SP) on the metal substrate. In this work, the generation of a convergent light beam via using the SP-locked SPR is proposed and investigated by computer simulations. The proposed structure is composed of an insulator-metal-insulator (IMI) substrate with chirped gratings on the substrate. The chirped gratings are designed such that a convergent beam containing a single wavelength is formed directly above the gratings when an electron bunch passes beneath the substrate. The wavelength of the convergent beam changes with the refractive index of dielectric layer of the IMI structure, which is determined by the frequency of SP on the IMI substrate excited by the electron bunch. Moreover, reversing the direction of electron bunch will make the emitted light from the proposed structure to switch from a convergent beam to a divergent beam. Finally, the formation of a convergent beam containing red, green and blue lights just above the chirped gratings is also demonstrated. This work offers potential applications in the fields of optical imaging, optical beam steering, holography, microdisplay, cryptography and light source.

Highlights

  • Optical beam steering is an important issue in nanoscale imaging[1]

  • To form a convergent spot at θ = 0° and R = 6 μm, the chirped gratings need to be designed such that different lights emitted from different positions all propagate toward the convergent spot

  • The proposed structure is composed of an IMI substrate with chirped gratings on the substrate

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Summary

Results

Dielectric films are set as 2.6, 2.1 and 1.7, respectively. The total lengths of the IMI structure and the buffer layer are both 10 μm. (The chirped gratings are placed at the center of the substrate). (a–c) Simulated contours of Fourier spectra of Hz fields as functions of emission wavelength and angle at the observation points for SPR emitted from the proposed structure in Fig. 1 with refractive indices of dielectric layers equal to 1.7 (λ = 457 nm), 2.1 (λ = 535 nm), and 2.6 (λ = 633 nm), respectively. 193, 190, 187, 184, 182, 180, 178, 176, 174, 173, 172 (the third section, total 11 values)

Discussion
Methods and Materials
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