2011
DOI: 10.1088/1367-2630/13/8/083013
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Optical characterization of charge transfer and bonding dimer plasmons in linked interparticle gaps

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Cited by 53 publications
(76 citation statements)
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“…Similarly, because of electron tunneling, the QP mode continuously evolves into a higher order charge transfer plasmon mode C2 before direct contact between the nanowires. Thus, already at positive S the nanowires are conductively connected showing characteristic charge transfer plasmon modes [48,[51][52][53]55,56]. For a dimer with a well established conductive contact at negative S, the C1 and C2 modes experience a blue shift with increasing overlap as also found in classical calculations [48,63].…”
Section: Coupled Nanowiressupporting
confidence: 63%
See 1 more Smart Citation
“…Similarly, because of electron tunneling, the QP mode continuously evolves into a higher order charge transfer plasmon mode C2 before direct contact between the nanowires. Thus, already at positive S the nanowires are conductively connected showing characteristic charge transfer plasmon modes [48,[51][52][53]55,56]. For a dimer with a well established conductive contact at negative S, the C1 and C2 modes experience a blue shift with increasing overlap as also found in classical calculations [48,63].…”
Section: Coupled Nanowiressupporting
confidence: 63%
“…The nanoparticles thus appear conductively connected prior to direct contact, and the transition between the non-touching and conductive contact regimes is continuous. In particular, the charge transfer plasmon associated with interparticle charge transfer [51][52][53][54][55][56][57] progressively emerges in the optical response of the system, as has been fully confirmed in recent experiments [28,29]. These quantum effects can be reproduced with the Quantum Corrected Model (QCM) [33] that treats the junction between the nanoparticles as an effective medium mimicking quantum effects within the classical local Maxwell theory [28,29].…”
Section: Introductionmentioning
confidence: 66%
“…For this reason, this longitudinal D mode has recently been termed the charge transfer plasmon mode in the context of close touching metallic nanoparticles. [20][21][22][23] Importantly, Figure 2 (a) demonstrates that, as predicted theoretically, [ 6 , 16 ] the effect of the D mode is to effectively broaden the ACS, leading to greater absorption at lower frequencies. Figure 2 (c) shows that, similarly to the longitudinal D-D mode, this resonance yields a strong ( ∼ 130 fold) fi eld enhancement in the narrow gap separating the two disks, above the contact point.…”
Section: Doi: 101002/adma201202003supporting
confidence: 61%
“…This BDP mode presents strongly localised charge densities of opposite sign and enormously enhanced local electromagnetic fields at the cavity. In contrast, when a conductive path is established between both particles of the dimer, a Charge Transfer Plasmon (CTP) mode is allowed, with current density crossing through the cavity, involving an oscillating distribution of net charge at every individual nanoparticle [13,14,17,18]. In most of the studies dealing with these effects, classical electrodynamical approaches have been applied.…”
Section: Introductionmentioning
confidence: 99%