2005 APS March Meeting
Monday–Friday, March 21–25, 2005;
Los Angeles, CA
Session V15: Focus Session: Plasmonics, Biological, Solar Cell QDs
11:15 AM–1:39 PM,
Thursday, March 24, 2005
LACC
Room: 405
Sponsoring
Unit:
FIAP
Chair: H. Atwater, Caltech
Abstract ID: BAPS.2005.MAR.V15.1
Abstract: V15.00001 : Semiconductor Quantum Dots in Metal Nanostructures*
11:15 AM–11:51 AM
Preview Abstract
Abstract
Author:
Mark Stockman
(Department of Physics and Astronomy, Georgia State University, Atlanta, GA 30303, USA)
We consider theory and available experimental data on optical and electronic
properties of nanostructures containing semiconductor nanocrystal quantum
dots (QDs) in a nano-proximity of metal surfaces and nanoparticles.
Remarkable properties of such systems are due to a strong coupling between
QD electrons and surface plasmons (SPs) and surface plasmon polaritons
(SPPs) of the metal.
Generally, the proximity to metal accelerates electronic transitions in the
quantum dots. However, dependent on QD transition frequency $\omega $ and
distance between QDs and the metal surface, and the size of the metal
nanostructure, there may be different scenarios of such interactions with
dramatically different effects.
\begin{enumerate}
\item For lower frequencies the QD transitions $\omega <\sim \omega _{SP} $, where $\omega _{SP} $ is a characteristic surface plasmon (SP) frequency, and $d\sim 1$ nm, the dominating interaction is that the excitation of localized SPs of the metal that undergo a strong Landau damping. This introduces a very fast Landau damping, efficiently damping the fluorescence of QDs.
\item For $\omega \sim \omega _{SP} $, $d>\sim 1$ nm and nanoscale size of the metal system, coherent excitation of SPs takes place. In this case, the metal system may work as a nano-antenna for QDs enhancing the dipole oscillator strength of QD transitions. In this case, one expect \textit{enhanced} luminescence of QDs, opposite to what takes place in case ($i)$. One can also expect the surface-enhanced Raman scattering (SERS) and strongly enhanced nonlinear effects such as CARS. One unique effect that is predicted in such systems is surface plasmon amplification by stimulated emission of radiation (spaser), which is similar to laser where the coherent accumulation of SPs in a single mode takes place.
\item For $\omega \sim \omega _{SP} $, $d>\sim 1$ nm, and macroscopic extension size of the metal system, besides SPs, the propagating modes of SPPs are excited. In this case, the metal system plays role of optical antenna that propagates the excitation of the quantum dots to the far zone. This leads to an increase of the fluorescence efficiency and intensity, and shortening of the fluorescence time.
\end{enumerate}
There are numerous potential applications of the QD/metal nanostructures
that we will be discussing.
*This work was supported by grants from the Chemical Sciences, Biosciences and Geosciences Division of the Office of Basic Energy Sciences, Office of Science, U.S. Department of Energy
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2005.MAR.V15.1