• Photonics Research
  • Vol. 10, Issue 4, 974 (2022)
Brian Slovick* and Josh Hellhake
Author Affiliations
  • Advanced Technology and Systems Division, SRI International, Menlo Park, California 94025, USA
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    DOI: 10.1364/PRJ.450937 Cite this Article Set citation alerts
    Brian Slovick, Josh Hellhake. Inverse design of invisibility cloaks using the optical theorem[J]. Photonics Research, 2022, 10(4): 974 Copy Citation Text show less
    Relative permittivity, scattered fields, total fields, and scattered intensity for a 0.5λ radius metal rod with (a) no cloak, (b) optimized 0.5λ thick cloak for an initial seed of ϵshell=3, and (c) optimized 0.5λ thick cloak for an initial seed of ϵshell=5.
    Fig. 1. Relative permittivity, scattered fields, total fields, and scattered intensity for a 0.5λ radius metal rod with (a) no cloak, (b) optimized 0.5λ thick cloak for an initial seed of ϵshell=3, and (c) optimized 0.5λ thick cloak for an initial seed of ϵshell=5.
    Relative permittivity, scattered fields, total fields, and scattered intensity for a 0.5λ radius metal rod with (a) no cloak, (b) optimized 0.25λ thick cloak for an initial seed of ϵshell=3, and (c) optimized 0.25λ thick cloak for an initial seed of ϵshell=5.
    Fig. 2. Relative permittivity, scattered fields, total fields, and scattered intensity for a 0.5λ radius metal rod with (a) no cloak, (b) optimized 0.25λ thick cloak for an initial seed of ϵshell=3, and (c) optimized 0.25λ thick cloak for an initial seed of ϵshell=5.
    Relative permittivity, scattered fields, total fields, and scattered intensity for an elliptical metal rod with 0.8λ and 0.4λ major and minor axes, respectively, with (a) no cloak, (b) optimized 0.2λ thick cloak for an initial seed of ϵshell=3, and (c) optimized 0.2λ thick cloak for an initial seed of ϵshell=5.
    Fig. 3. Relative permittivity, scattered fields, total fields, and scattered intensity for an elliptical metal rod with 0.8λ and 0.4λ major and minor axes, respectively, with (a) no cloak, (b) optimized 0.2λ thick cloak for an initial seed of ϵshell=3, and (c) optimized 0.2λ thick cloak for an initial seed of ϵshell=5.
    Cross section of the uncloaked structure in Fig. 1(a) and the optimized cloak in Fig. 1(b) as a function of (a) wavelength and (b) angle of incidence.
    Fig. 4. Cross section of the uncloaked structure in Fig. 1(a) and the optimized cloak in Fig. 1(b) as a function of (a) wavelength and (b) angle of incidence.
    Brian Slovick, Josh Hellhake. Inverse design of invisibility cloaks using the optical theorem[J]. Photonics Research, 2022, 10(4): 974
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