Matches in SemOpenAlex for { <https://semopenalex.org/work/W2996153886> ?p ?o ?g. }
- W2996153886 endingPage "411957" @default.
- W2996153886 startingPage "411957" @default.
- W2996153886 abstract "In the present paper we report the optical response of an ordered array of silver (Ag) nanoparticles (NPs) using the uniaxial LiNbO3 as a model case. We investigate the anisotropic effects on the effective dielectric tensor taking into account the charges interaction of particles. The Ag NPs dielectric function is described through a modified Drude model whereas the LiNbO3 dielectric functions are deduced from their experimentally established Sellmeier equations. The effective dielectric tensor components of the ensemble aggregates of Ag NPs and uniaxial LiNbO3 crystal are treated through the extended Maxwell–Garnett approximation. Following the asymmetric behaviour of uniaxial crystals, Ag NPs are sited in the ordinary plane of the crystal, giving rise to different responses in the x, y and z directions of applied electric field. Real and imaginary parts of the effective dielectric tensor components of the aggregate ensemble are investigated in terms of different structural parameters, such as the interparticle spacings, the NPs filling factor and sizes of spherically embedded nanoparticles. We demonstrate that an adequate choice of structural parameters such as NPs sizes, interparticle separation gaps or the filling factor can determine the optical properties of layered Ag–embedded uniaxial crystals such as LiNbO3. We show that the negative epsilon (NE) condition is satisfied from a critical size of Ag NPs when the filling factor and the interparticles distances (a and b) have particular values. This condition defines an interval of energies, called NE range, which clearly depend on values of structural parameters defined in the model. This NE range shows some type of bandwidth anisotropy when it is compared among the x-, y-, z- and xy-components of the effective dielectric tensor. We analyze some anisotropic features such as the bandwidth and shift resonance energies in the real and imaginary parts of the dielectric tensor when structural parameters change." @default.
- W2996153886 created "2019-12-26" @default.
- W2996153886 creator A5032019341 @default.
- W2996153886 creator A5082196249 @default.
- W2996153886 creator A5086697925 @default.
- W2996153886 date "2020-03-01" @default.
- W2996153886 modified "2023-10-01" @default.
- W2996153886 title "Dielectric tensor of a rectangular arrangement of Ag nanoparticles in anisotropic <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline id=d1e396 altimg=si15.svg><mml:mrow><mml:mi>L</mml:mi><mml:mi>i</mml:mi><mml:mi>N</mml:mi><mml:mi>b</mml:mi><mml:msub><mml:mrow><mml:mi>O</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>: Analysis of the negative epsilon conditions" @default.
- W2996153886 cites W1974144067 @default.
- W2996153886 cites W1978906881 @default.
- W2996153886 cites W1984251057 @default.
- W2996153886 cites W1987880468 @default.
- W2996153886 cites W2001284909 @default.
- W2996153886 cites W2004439326 @default.
- W2996153886 cites W2004468469 @default.
- W2996153886 cites W2013530408 @default.
- W2996153886 cites W2016927087 @default.
- W2996153886 cites W2024538745 @default.
- W2996153886 cites W2025628651 @default.
- W2996153886 cites W2025864484 @default.
- W2996153886 cites W2057392849 @default.
- W2996153886 cites W2061879399 @default.
- W2996153886 cites W2067969923 @default.
- W2996153886 cites W2082544111 @default.
- W2996153886 cites W2087572685 @default.
- W2996153886 cites W2087972832 @default.
- W2996153886 cites W2099280870 @default.
- W2996153886 cites W2132934967 @default.
- W2996153886 cites W2142770987 @default.
- W2996153886 cites W2145627618 @default.
- W2996153886 cites W2164930156 @default.
- W2996153886 cites W2315712994 @default.
- W2996153886 cites W2410624667 @default.
- W2996153886 cites W2429360284 @default.
- W2996153886 cites W2507494493 @default.
- W2996153886 cites W2642815282 @default.
- W2996153886 cites W2893803800 @default.
- W2996153886 cites W34777478 @default.
- W2996153886 doi "https://doi.org/10.1016/j.physb.2019.411957" @default.
- W2996153886 hasPublicationYear "2020" @default.
- W2996153886 type Work @default.
- W2996153886 sameAs 2996153886 @default.
- W2996153886 citedByCount "7" @default.
- W2996153886 countsByYear W29961538862020 @default.
- W2996153886 countsByYear W29961538862021 @default.
- W2996153886 countsByYear W29961538862023 @default.
- W2996153886 crossrefType "journal-article" @default.
- W2996153886 hasAuthorship W2996153886A5032019341 @default.
- W2996153886 hasAuthorship W2996153886A5082196249 @default.
- W2996153886 hasAuthorship W2996153886A5086697925 @default.
- W2996153886 hasConcept C120665830 @default.
- W2996153886 hasConcept C121332964 @default.
- W2996153886 hasConcept C128258110 @default.
- W2996153886 hasConcept C133386390 @default.
- W2996153886 hasConcept C15336307 @default.
- W2996153886 hasConcept C155281189 @default.
- W2996153886 hasConcept C155672457 @default.
- W2996153886 hasConcept C159985019 @default.
- W2996153886 hasConcept C171250308 @default.
- W2996153886 hasConcept C192562407 @default.
- W2996153886 hasConcept C199360897 @default.
- W2996153886 hasConcept C204323151 @default.
- W2996153886 hasConcept C2524010 @default.
- W2996153886 hasConcept C26873012 @default.
- W2996153886 hasConcept C2781285689 @default.
- W2996153886 hasConcept C33923547 @default.
- W2996153886 hasConcept C3756478 @default.
- W2996153886 hasConcept C41008148 @default.
- W2996153886 hasConcept C49040817 @default.
- W2996153886 hasConcept C85725439 @default.
- W2996153886 hasConceptScore W2996153886C120665830 @default.
- W2996153886 hasConceptScore W2996153886C121332964 @default.
- W2996153886 hasConceptScore W2996153886C128258110 @default.
- W2996153886 hasConceptScore W2996153886C133386390 @default.
- W2996153886 hasConceptScore W2996153886C15336307 @default.
- W2996153886 hasConceptScore W2996153886C155281189 @default.
- W2996153886 hasConceptScore W2996153886C155672457 @default.
- W2996153886 hasConceptScore W2996153886C159985019 @default.
- W2996153886 hasConceptScore W2996153886C171250308 @default.
- W2996153886 hasConceptScore W2996153886C192562407 @default.
- W2996153886 hasConceptScore W2996153886C199360897 @default.
- W2996153886 hasConceptScore W2996153886C204323151 @default.
- W2996153886 hasConceptScore W2996153886C2524010 @default.
- W2996153886 hasConceptScore W2996153886C26873012 @default.
- W2996153886 hasConceptScore W2996153886C2781285689 @default.
- W2996153886 hasConceptScore W2996153886C33923547 @default.
- W2996153886 hasConceptScore W2996153886C3756478 @default.
- W2996153886 hasConceptScore W2996153886C41008148 @default.
- W2996153886 hasConceptScore W2996153886C49040817 @default.
- W2996153886 hasConceptScore W2996153886C85725439 @default.
- W2996153886 hasFunder F4320313831 @default.
- W2996153886 hasFunder F4320322930 @default.
- W2996153886 hasLocation W29961538861 @default.
- W2996153886 hasOpenAccess W2996153886 @default.
- W2996153886 hasPrimaryLocation W29961538861 @default.
- W2996153886 hasRelatedWork W1964632126 @default.
- W2996153886 hasRelatedWork W2016400634 @default.
- W2996153886 hasRelatedWork W2028255301 @default.