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dc.contributor.authorTANDON, BHARATen_US
dc.contributor.authorAgrawal, Ankiten_US
dc.contributor.authorHeo, Sungyeonen_US
dc.contributor.authorMilliron, Delia J.en_US
dc.date.accessioned2019-04-25T07:00:12Z
dc.date.available2019-04-25T07:00:12Z
dc.date.issued2019-02en_US
dc.identifier.citationNano Letters, 19(3), 2012-2019.en_US
dc.identifier.issn1530-6984en_US
dc.identifier.issn1530-6992en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/2450-
dc.identifier.urihttps://doi.org/10.1021/acs.nanolett.9b00079en_US
dc.description.abstractDegenerately doped semiconductor nanocrystals (NCs) exhibit strong light-matter interactions due to localized surface plasmon resonance (LSPR) in the near- to mid-infrared region. Besides being readily tuned through dopant concentration introduced during synthesis, this LSPR can also be dynamically modulated by applying an external electrochemical potential. This characteristic makes these materials candidates for electro-chromic window applications. Here, using prototypical doped indium oxide NCs as a model system, we find that the extent of electrochemical modulation of LSPR frequency is governed by the depletion width and the extent of inter-NC LSPR coupling, which are indirectly controlled by the dopant density, size, and packing density of the NCs. The depletion layer is a near-surface region with a sharply reduced free carrier population that occurs whenever the surface potential lies below the Fermi level. Changes in the depletion width under applied bias substantially control the spectral modulation of the LSPR of individual NCs and also modify the inter-NC LSPR coupling, which additionally modulates the LSPR absorption on the NC film scale. Here, we show that both of these effects must be considered primary factors in determining the extent of LSPR frequency modulation and that the dominant factor depends on NC size. For a constant doping concentration, depletion effects govern LSPR modulation for smaller NCs, while LSPR coupling is prevalent in larger NCs. Consequently, as the size of the NCs is increased while keeping the doping concentration constant, we observe a reversal in the sign of the LSPR frequency modulation from positive to negative.en_US
dc.language.isoenen_US
dc.publisherAmerican Chemical Societyen_US
dc.subjectSemiconductor nanocrystalsen_US
dc.subjectIndium oxideen_US
dc.subjectlocalized surface plasmon resonanceen_US
dc.subjectLSPR modulationen_US
dc.subjectDepletionen_US
dc.subjectLSPR couplingen_US
dc.subjectTOC-APR-2019en_US
dc.subject2019en_US
dc.titleCompetition between Depletion Effects and Coupling in the Plasmon Modulation of Doped Metal Oxide Nanocrystalsen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Chemistryen_US
dc.identifier.sourcetitleNano Lettersen_US
dc.publication.originofpublisherForeignen_US
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