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Optical Limitation induced by Gold Clusters. 1. Size Effect5 W5 j, E( o$ d$ [3 @: y
Lionel Francüois, Mehran Mostafavi,* and Jacqueline Belloni4 K7 U" K$ j ]+ |7 E
Laboratoire de Chimie Physique, UMR 8610 CNRS, UniVersite´ Paris-Sud, 91405 Orsay, Cedex, France
4 M! v7 ~) c0 g. G6 K' yJean-Francüois Delouis and Jacques Delaire6 x4 b% C# V& ?* q( T
Laboratoire de Photophysique et Photochimie Supramole´culaires et Macromole´culaires, UMR 8531,8 ~- k9 n9 Q$ N& ^5 q: T( `$ }
Ecole Normale Supe´rieure de Cachan, 94235 Cachan Cedex, France
8 z8 `+ ]0 O, NPatrick Feneyrou: ?# L9 b3 ^# o" E8 Y' C) Y
Laboratoire Central de Recherches, Thomson-CSF, Domaine de CorbeVille, 91404 Orsay Cedex, France
* D: _- y4 G/ t) ~! U4 u N' eReceiVed: December 20, 1999; In Final Form: March 8, 2000
! u/ ~9 y' r' b; C6 p! a5 E, a, {The nonlinear optical response of gold particles (with 2.5, 9, or 15 nm radius) prepared by ç-radiolysis in
/ V, O( E- S7 M8 z, Jwater solution and stabilized by poly(vinyl alcohol) is size-dependent. The 2.5 nm clusters do not limit light
2 q' l2 o0 M+ e1 R ~transmission even at very high fluence of nanosecond laser pulses, while the larger clusters strongly limit the
/ Y0 L5 `! j g. vlaser beam transmission at 530 nm. The threshold of limitation and the amplitude depend on the size of the b8 z2 G ^% [
particles. The rise of the optical limiting effect is measured by picosecond laser spectroscopy. For the largest7 B P5 _ \: I/ O1 x! A/ P) w3 S: N
particles, it lasts 1 ns. The limitation effect is attributed to large light-scattering centers induced by the pulse6 W9 R5 e- L8 S7 s6 \
around the initial particles. |
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