Upper bounds on absorption and scattering

A general framework for determining fundamental bounds in nanophotonics is introduced in this paper. The theory is based on convex optimization of dual problems constructed from operators generated by electromagnetic integral equations. The optimized variable is a contrast current defined within a p...

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Main Authors: Mats Gustafsson, Kurt Schab, Lukas Jelinek, Miloslav Capek
Format: Article
Language:English
Published: IOP Publishing 2020-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/ab83d3
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author Mats Gustafsson
Kurt Schab
Lukas Jelinek
Miloslav Capek
author_facet Mats Gustafsson
Kurt Schab
Lukas Jelinek
Miloslav Capek
author_sort Mats Gustafsson
collection DOAJ
description A general framework for determining fundamental bounds in nanophotonics is introduced in this paper. The theory is based on convex optimization of dual problems constructed from operators generated by electromagnetic integral equations. The optimized variable is a contrast current defined within a prescribed region of a given material constitutive relations. Two power conservation constraints analogous to the optical theorem are utilized to tighten the bounds and to prescribe either losses or material properties. Thanks to the utilization of matrix rank-1 updates, modal decompositions, and model order reduction techniques, the optimization procedure is computationally efficient even for complicated scenarios. No dual gaps are observed. The method is well-suited to accommodate material anisotropy and inhomogeneity. To demonstrate the validity of the method, bounds on scattering, absorption, and extinction cross sections are derived first and evaluated for several canonical regions. The tightness of the bounds is verified by comparison to optimized spherical nanoparticles and shells. The next metric investigated is bi-directional scattering studied closely on a particular example of an electrically thin slab. Finally, the bounds are established for Purcell’s factor and local field enhancement where a dimer is used as a practical example.
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spelling doaj.art-44cf87a6484d42b1b3dc888d2457e99c2023-08-08T15:29:56ZengIOP PublishingNew Journal of Physics1367-26302020-01-0122707301310.1088/1367-2630/ab83d3Upper bounds on absorption and scatteringMats Gustafsson0https://orcid.org/0000-0003-4362-5716Kurt Schab1https://orcid.org/0000-0002-4228-9856Lukas Jelinek2https://orcid.org/0000-0002-1163-9059Miloslav Capek3https://orcid.org/0000-0002-7442-889XDepartment of Electrical and Information Technology, Lund University , Lund, SwedenDepartment of Electrical Engineering, Santa Clara University , Santa Clara, United States of AmericaDepartment of Electromagnetic Field, Czech Technical University in Prague , Prague, Czech RepublicDepartment of Electromagnetic Field, Czech Technical University in Prague , Prague, Czech RepublicA general framework for determining fundamental bounds in nanophotonics is introduced in this paper. The theory is based on convex optimization of dual problems constructed from operators generated by electromagnetic integral equations. The optimized variable is a contrast current defined within a prescribed region of a given material constitutive relations. Two power conservation constraints analogous to the optical theorem are utilized to tighten the bounds and to prescribe either losses or material properties. Thanks to the utilization of matrix rank-1 updates, modal decompositions, and model order reduction techniques, the optimization procedure is computationally efficient even for complicated scenarios. No dual gaps are observed. The method is well-suited to accommodate material anisotropy and inhomogeneity. To demonstrate the validity of the method, bounds on scattering, absorption, and extinction cross sections are derived first and evaluated for several canonical regions. The tightness of the bounds is verified by comparison to optimized spherical nanoparticles and shells. The next metric investigated is bi-directional scattering studied closely on a particular example of an electrically thin slab. Finally, the bounds are established for Purcell’s factor and local field enhancement where a dimer is used as a practical example.https://doi.org/10.1088/1367-2630/ab83d3boundsscatteringfield enhancementabsorptionplasmonicsconvex optimization
spellingShingle Mats Gustafsson
Kurt Schab
Lukas Jelinek
Miloslav Capek
Upper bounds on absorption and scattering
New Journal of Physics
bounds
scattering
field enhancement
absorption
plasmonics
convex optimization
title Upper bounds on absorption and scattering
title_full Upper bounds on absorption and scattering
title_fullStr Upper bounds on absorption and scattering
title_full_unstemmed Upper bounds on absorption and scattering
title_short Upper bounds on absorption and scattering
title_sort upper bounds on absorption and scattering
topic bounds
scattering
field enhancement
absorption
plasmonics
convex optimization
url https://doi.org/10.1088/1367-2630/ab83d3
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