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页数:26页
时间:2019-03-11
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1、Chapter15TheoreticalMethodsinNano-OpticsAmajorprobleminnano-opticsisthedeterminationofelectromagneticfielddistri-butionsnearnanoscalestructuresandtheassociatedradiationproperties.Asolidtheoreticalunderstandingoffielddistributionsholdspromisefornew,optimizedde-signsofnear-fieldopticaldevi
2、ces,inparticularbyexploitationoffield-enhancementeffectsandfavorabledetectionschemes.Calculationsoffielddistributionsarealsonecessaryforimagereconstructionpurposes.Fieldsnearnanoscalestructureshaveoftentobereconstructedfromexperimentallyaccessiblefarfielddata.However,mostcommonlytheinvers
3、escatteringproblemcannotbesolvedinauniquewayandcalcu-lationsoffield-distributionsareneededtoprovidepriorknowledgeaboutsourceandscatteringobjectsandtorestrictthesetofpossiblesolutions.AnalyticalsolutionsofMaxwell’sequationsprovideagoodtheoreticalunderstand-ingbutcanbeobtainedforsimplepr
4、oblemsonly.Otherproblemshavetobestronglysimplified.Ontheotherhand,apurenumericalanalysisallowstohandlecomplexproblemsbydiscretizationofspaceandtimebutcomputationalrequirements(usu-allygivenbycputimeandmemory)limitthesizeoftheproblemandtheaccuracyofresultsisoftenunknown.Theadvantageofpu
5、renumericalmethods,suchasthefinite-differencetime-domain(FDTD)methodorthefinite-element(FE)method,istheeaseofimplementation.Wewillnotreviewthesepurenumericaltechniquessincetheyarewelldocumentedintheliterature.Insteadwewillreviewtwocommonlyusedsemi-analyticalmethodsinnano-optics:themultip
6、le-multipolemethod(MMP)andthevolumeintegralmethod.Thelatterexistsindifferentimplementationssuchasthecoupled-dipolemethod,thedipole-dipoleapproximation,orthemethodofmo-ments.BothMMPandthevolumeintegralmethodaresemiclassicalmethodssincetheyrenderananalyticalexpansionfortheelectromagnetic
7、fieldbynumericalmeans.12CHAPTER15.THEORETICALMETHODSINNANO-OPTICS15.1TheMultipleMultipoleMethodThemultiplemultipolemethod(MMP)isacompromisebetweenapureanalyticalandapurenumericalapproach.Itisawell-establishedtechniqueforsolvingMaxwell’sequationsinarbitrarilyshaped,isotropic,linearandpi
8、ecewi
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