Excitation and Dispersion Characteristics of Transverse Magnetic Supermodes in Plasmonic Optical Fibers

We investigate the dispersion characteristics of the transverse magnetic (TM) guided supermodes (sTM<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">01</inf>, sTM<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">02</inf>, and a<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b</inf>) in a tapered, metal-coated optical fiber core. The structure consists of a fiber core coated with a 25 nm gold film, tapered from an 8.2 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\boldsymbol{\mu} \mathbf{m}$</tex> diameter down to 0.4 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\boldsymbol{\mu} \mathbf{m}$</tex>. We use a cascaded eigenmode expansion algorithm to quantify the evolution of the supermodes and identify two primary loss mechanisms: i) catastrophic coupling loss when the fundamental sTM<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">01</inf> mode cuts off, and ii) inherent propagation loss due to the plasmonic nature of the modes.

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Published
2025-05-20
DOI
https://doi.org/10.1109/pn66844.2025.11097086
Primary Topic
Plasmonic and Surface Plasmon Research
Type
article
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article

Excitation and Dispersion Characteristics of Transverse Magnetic Supermodes in Plasmonic Optical Fibers

Binny Jind, Pierre Berini
2 links
Plasmonic and Surface Plasmon Research
article

Excitation and Dispersion Characteristics of Transverse Magnetic Supermodes in Plasmonic Optical Fibers

Binny Jind, Pierre Berini
article en

Abstract

We investigate the dispersion characteristics of the transverse magnetic (TM) guided supermodes (sTM<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">01</inf>, sTM<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">02</inf>, and a<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b</inf>) in a tapered, metal-coated optical fiber core. The structure consists of a fiber core coated with a 25 nm gold film, tapered from an 8.2 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\boldsymbol{\mu} \mathbf{m}$</tex> diameter down to 0.4 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\boldsymbol{\mu} \mathbf{m}$</tex>. We use a cascaded eigenmode expansion algorithm to quantify the evolution of the supermodes and identify two primary loss mechanisms: i) catastrophic coupling loss when the fundamental sTM<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">01</inf> mode cuts off, and ii) inherent propagation loss due to the plasmonic nature of the modes.

University of Ottawa (CA)
Natural Sciences and Engineering Research Council of Canada
Openalex Percentile: Top 82%
Plasmonic and Surface Plasmon Research
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