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Untitled - IAP/TU Wien - Technische Universität Wien

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71st IUVSTA Workshop<br />

Effects of sudden photo electron-hole pair creation on the induced surface plasmon excitations<br />

in cylindrical nanorods<br />

Juana L. Gervasoni, 1,* !"#$%&$'()*+ ,<br />

1 !"#$%&'()*+,&-$'*.)/,)#*"/0*1/2,$,3,&*!"%2)$#&4*5.67+8*+9:*!32,$%%&*;:*?@==8*!"#$%&'()A*B$&*6)C#&4*<br />

+#C)/,$/":*+%2&*-)-D)#*&E*,()*.&/2)F&*6"'$&/"%*0)*1/9)2,$C"'$&/)2*.$)/,$E$'"2*G*H)'/&%&C$'"2*5.I61.7H84*<br />

+#C)/,$/".<br />

2 1/2,$,3,)*&E*63'%)"#*B)2)"#'(4*J+K*5LH+*+HILM184*N?O'*!)-*,)#4*JP@=QR*S)D#)')/4*J3/C"#G.<br />

*gervason@cab.cnea.gov.ar<br />

In this work we study the effect of the excitation of surface plasmons in a metallic cylindrical<br />

nanorod by a suddenly created electron-hole pair, using a classical model for the emerging electron and a<br />

quantum-mechanical model for the plasmon field in the cylinder [1]. The emitted electron and the hole interact<br />

independently with the free electrons in the metallic Al, generating electron density oscillations. Two different<br />

trajectories for the emerging electron (parallel to the axis and radial) are studied in an aluminum nanorod. The<br />

average number of excited plasmons indicates how important the role of the hole in the excitation process is.<br />

We found that the results can be very different according to the trajectory of the emerging electron. We also<br />

found that the separation of the intrinsic and extrinsic process is sometimes not applicable.<br />

References<br />

[1] J.A. García Gallardo, J. L. Gervasoni, L. Kövér. Vacuum, 84 (2010) 258.<br />

35

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