Abstract

A nanoscale Bragg grating reflector based on the defect metal-insulator-metal (MIM) waveguide is developed and numerically simulated by using the finite element method (FEM). The MIM-based structure promises a highly tunable broad stop-band in transmission spectra. The narrow transmission window is shown to appear in the previous stop-band by changing the certain geometrical parameters. The central wavelengths can be controlled easily by altering the geographical parameters. The development of surface plasmon polarition (SPP) technology in metallic waveguide structures leads to more possibilities of controlling light at deep sub-wavelengths. Its attractive ability of breaking the diffraction limit contributes to the design of optical sensors.

Highlights

  • Surface plasmon polaritions (SPPs) are mixed electromagnetic waves confining at the metal surface, which results from electromagnetic waves coupling to free electron oscillations

  • The MIM Bragg reflectors have a wide range of applications in optical communication fields such as optical filters [9], which have been theoretically proposed and experimentally demonstrated, single-cavity and multi-cavity structures filters [10], and tunable channel drop filters [11]

  • In order to realize the sensing application of the proposed MIM plasmonic Bragg grating, we

Read more

Summary

Introduction

Surface plasmon polaritions (SPPs) are mixed electromagnetic waves confining at the metal surface, which results from electromagnetic waves coupling to free electron oscillations. The MIM Bragg reflectors have a wide range of applications in optical communication fields such as optical filters [9], which have been theoretically proposed and experimentally demonstrated, single-cavity and multi-cavity structures filters [10], and tunable channel drop filters [11]. Due to their unique feature of subwavelength of confinement, optical sensors are another important application of communication that can be controlled by the width [12,13], effective refractive index [14], force, and so on. Of the proposed structure shows a promising future for various applications

Structures and Theoretical Analysis
The structure of of the the MIM
Results and Discussion
Transmission spectraofofthe theMIM-based
24 Figure in Figure
Characterization of thedifferent
Conclusions
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.