CLC number: O441; TN75
On-line Access:
Received: 2005-09-05
Revision Accepted: 2005-10-10
Crosschecked: 0000-00-00
Cited: 2
Clicked: 5369
Simovski C.R., Viitanen A.J., Tretyakov S.A.. A resonator mode in linear arrays of silver spheres and cylinders[J]. Journal of Zhejiang University Science A, 2006, 7(1): 29-33.
@article{title="A resonator mode in linear arrays of silver spheres and cylinders",
author="Simovski C.R., Viitanen A.J., Tretyakov S.A.",
journal="Journal of Zhejiang University Science A",
volume="7",
number="1",
pages="29-33",
year="2006",
publisher="Zhejiang University Press & Springer",
doi="10.1631/jzus.2006.A0029"
}
%0 Journal Article
%T A resonator mode in linear arrays of silver spheres and cylinders
%A Simovski C.R.
%A Viitanen A.J.
%A Tretyakov S.A.
%J Journal of Zhejiang University SCIENCE A
%V 7
%N 1
%P 29-33
%@ 1673-565X
%D 2006
%I Zhejiang University Press & Springer
%DOI 10.1631/jzus.2006.A0029
TY - JOUR
T1 - A resonator mode in linear arrays of silver spheres and cylinders
A1 - Simovski C.R.
A1 - Viitanen A.J.
A1 - Tretyakov S.A.
J0 - Journal of Zhejiang University Science A
VL - 7
IS - 1
SP - 29
EP - 33
%@ 1673-565X
Y1 - 2006
PB - Zhejiang University Press & Springer
ER -
DOI - 10.1631/jzus.2006.A0029
Abstract: A transversal mode with zero group velocity and non-zero phase velocity that can exist in chains of silver nano-spheres in the optical frequency range was theoretically studied. It is shown that the external source radiating a narrow-band non-monochromatic signal can excite in the chain a mixture of standing and slowly travelling waves. The standing wave component (named as resonator mode) is strongly dominating. The physical reason of such a regime is a sign-varying distribution of power flux over the cross section of the chain. This situation is similar to the scenario of the propagation of a wave along the boundary between the right-handed and left-handed media where the spatial distribution of the light intensity is vortex. However, in the present case there is no boundary between media and the boundary between the positive and negative power fluxes is a cylindric tube in free space whose axis is the axis of the chain.
[1] Felsen, L.B., Marcuvitz, N., 1994. Radiation and Scattering of Waves. IEEE Press, New York.
[2] Girard, C., Dereux, A., Martin, O.J.F., Devel, M., 1994. Tailoring the transmittance of integrated optical waveguides with short metallic nanoparticle chains. Phys. Rev. B, 50:467-474.
[3] Kreibig, U., 1970. Optical constant of silver. Z. Physik, 234:307-309.
[4] Krenn, J.R., Wolf, R., Leitner, A., Aussenegg, F.R., 1997. Electromagnetic energy transport via linear chains of silver nanoparticles. Opt. Commun., 137:46-47.
[5] Krenn, J.R., Dereux, A., Weeber, J.C., Bourillot, E., Lacroute, Y., Goudonnet, J.P., Schider, G., Gotschy, W., Leitner, A., Aussenegg, F.R., Girard, C., 1999. Squeezing the optical near-field zone by plasmon coupling of metallic nanoparticles. Phys. Rev. Lett., 82:2590-2593.
[6] Sareni, B., 1996. Effective dielectric constant of periodic composite materials. Journal of Applied Physics, 80:1688-1696.
[7] Tretyakov, S.A., Viitanen, A.J., 2000. Line of periodically arranged passive dipole scatterers. Electrical Engineering, Archiv für Elektrotechnik, 82:353-361.
[8] Viitanen, A.J., Tretyakov, S.A., Simovski, C.R., 2005. Metawaveguide Formed by a Line of Plasmonic Nanoparticles. Proc. OSA Annual Conf. NPIS (Nanophotonics for Information Systems). San Diego, USA, p.484-487.
[9] Weber, W.H., Ford, G.M., 2004. Propagation of optical excitations by dipolar interactions in metal nanoparticle chains. Physical Review B, 70(12):125429(1-8).
Open peer comments: Debate/Discuss/Question/Opinion
<1>