Title: Nanoconfined Chemistry
1Computational Nanophotonics -- S. K. Gray
2Computational Nanophotonics Stephen K.
GrayChemistry DivisionArgonne National
LaboratoryArgonne, IL 60439gray_at_tcg.anl.govTel
630-252-3594
3Motivation
- Wish to control light or electromagnetic energy
in nano-sized optical devices - Problem optical light has wavelength gtgt 1nm
- Possible Solution
- - use near-field coupling of light
- with surface plasmons of
- metal nanoparticles
- gt arrays of metal nanoparticles
- become photonic devices
- gt steady or pulsed modes
- of illumination
surface-plasmon resonance in Au nanoparticles
4Excitation Transfer in Nanophotonics
Want Simulations to Guide Experiment
- arrays of metal nanoparticles substrate
represented by - spatially varying dielectric constant
-
- discretized fields E and H on 3D grids
-
- finite difference solution to Maxwells (curl)
equations for - time and spatial dependence of E and H fields
5Finite Difference Time Domain (FDTD) Method
- Maxwells PDEs ,
-
- outside nanoparticle inside
nanoparticle - ?E(x,t)/?t ? x H(x,t)/e(x) ?E(x,t)/?t ?
x H(x,t) - J(x,t)/e8 - ?H(x,t)/?t -? x E(x,t)/µo ?H(x,t)/?t
-? x E(x,t)/µo - ?J(x,t)/?t eowp2 E(x,t)/µo
-
-nJ(x,t) - are discretized in space and time in general,
6 or more components - are represented on a 3D spatial grid and
propagated in discrete time - steps
6FDTD Basics Yee Algorithm based on staggered
space and time grids
Space
- Each E component surrounded by 4 H components
- Each H component surrounded by 4 E components
7E and H Leapfrog in time
8More Explicitly Continuous Equations such as
9Get Replaced by Equations Like
10Current ANL Calculations
- 2D uniform grids (2000 x 2000) over 10000 time
steps - Silver nanowire (nanoscale radius infinite
cylinder) arrays considered - Variety of array configurations examined
11Example pulse of vertically polarized, 400 nm
light shows 100 nm scale localization when
passing (left to right) through a funnel
configuration of 30 nm diameter silver
nanowiresS. K. Gray and T. Kupka, Phys. Rev. B,
submitted (2003).
600 nm
0
0
600 nm
12Future Work Includes
- 3D Extensions for arbitrary shapes
- The FD algorithm parallelization
13Some Useful References Quinten et al., Optics
Letters 23, 1331 (1998) Maier et al., Advanced
Materials 13, 1501 (2001) Maier et al., Appl.
Phys. Lett. 81, 1714 (2002) Krenn et al.,
Europhys. Lett. 60, 663 (2002) Kottmann and
Martin, Optics Express 12, 655 (2001)