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Optical Limitation induced by Gold Clusters. 1. Size Effect
# [7 n: G8 Y( E' }6 [4 ]% MLionel Francüois, Mehran Mostafavi,* and Jacqueline Belloni. m/ _( s# h% Z( J" ?9 K
Laboratoire de Chimie Physique, UMR 8610 CNRS, UniVersite´ Paris-Sud, 91405 Orsay, Cedex, France
2 p2 C+ W/ B& l& D) n' h2 pJean-Francüois Delouis and Jacques Delaire; F9 H$ y2 q* u- B7 V: }
Laboratoire de Photophysique et Photochimie Supramole´culaires et Macromole´culaires, UMR 8531,2 w6 W b/ H2 W1 ?# N
Ecole Normale Supe´rieure de Cachan, 94235 Cachan Cedex, France
/ g+ m1 s8 }+ mPatrick Feneyrou7 y! E! S% Q" K- ]
Laboratoire Central de Recherches, Thomson-CSF, Domaine de CorbeVille, 91404 Orsay Cedex, France
7 @% Z- d: x- p0 _- i! p k4 _, VReceiVed: December 20, 1999; In Final Form: March 8, 20000 n! L) E' C" ?/ w3 }
The nonlinear optical response of gold particles (with 2.5, 9, or 15 nm radius) prepared by ç-radiolysis in+ N6 f+ o) [9 s ?2 a
water solution and stabilized by poly(vinyl alcohol) is size-dependent. The 2.5 nm clusters do not limit light! V' z8 e! X, i( W- E" H
transmission even at very high fluence of nanosecond laser pulses, while the larger clusters strongly limit the
8 n+ m c- [3 ]0 G5 Wlaser beam transmission at 530 nm. The threshold of limitation and the amplitude depend on the size of the* X0 t6 {+ S6 I" N( R/ W, c
particles. The rise of the optical limiting effect is measured by picosecond laser spectroscopy. For the largest
9 N4 D2 m" J! s( e( R6 ]/ rparticles, it lasts 1 ns. The limitation effect is attributed to large light-scattering centers induced by the pulse
" D5 y$ k9 d/ F/ U+ r1 V; [6 b& naround the initial particles. |
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