APS March Meeting 2010
Volume 55, Number 2
Monday–Friday, March 15–19, 2010;
Portland, Oregon
Session Z2: Plasmonic Nanogaps: From Single Molecule Sensing to Light Manipulation and Beyond
11:15 AM–2:15 PM,
Friday, March 19, 2010
Room: Oregon Ballroom 202
Sponsoring
Unit:
DCMP
Chair: Zhenyu Zhang, Oak Ridge National Laboratory
Abstract ID: BAPS.2010.MAR.Z2.2
Abstract: Z2.00002 : Quantum description of plasmons in strongly coupled metallic nanostructures
11:51 AM–12:27 PM
Preview Abstract
Abstract
Author:
Peter Nordlander
(Rice University)
The plasmonic couplings between closely positioned metallic
nanoparticles can induce extraordinary large electric field
enhancements in the junctions between the particles of
relevance for surface enhanced spectroscopies such as SERS.[1]
Such plasmonic couplings can also lead to plasmonic
interference and coherence effects that manifest themselves as
narrow Fano resonances in the optical spectra with
extraordinary sensitivities to their dielectric environment.[2]
Until very recently, the modeling of the plasmonic response of
closely coupled metallic nanoparticles has been made using
classical approaches neglecting quantum mechanical effects such
as electron tunneling between the particles and screening due
to the finite electron density in the junction. In this talk we
will present a fully quantum mechanical investigation of the
plasmonic response of two coupled metallic nanoparticles as a
function of interparticle separation.[3] We identify three
distinct regimes of interaction. In the classical regime for
separations larger than 1 nm, the nanoparticles remain neutral
and the plasmonic response is well described using classical
theory. In the cross-over regime for separations between 0.5
and 1nm, electrons begin to tunnel between the nanoparticles
and a reduction of the plasmonic couplings and field
enhancements result. In the conductive regime for separations
smaller than 0.5nm, a large conductive overlap is established
between the two particles and a blue-shifted Charge Transfer
Plasmon (CTP) emerges.[4] The CTP is a collective plasmon mode
which both includes a polarization of the electron distribution
of each individual nanoparticle and a significant electron
current between the two particles.
[1] F. Le et al., ACS Nano 2(2008)707-718
[3] N.A. Mirin, K. Bao, and P. Nordlander, J. Phys. Chem. A 113
(2009)4028-4034
[3] J. Zuloaga, E. Prodan, and P. Nordlander, Nano Lett. 9(2009)
887-891
[4] J.B. Lassiter et al., Nano Lett. 8(2008)1812-1816
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2010.MAR.Z2.2