Abstracts - Dipartimento di Elettronica Applicata
Abstracts - Dipartimento di Elettronica Applicata
Abstracts - Dipartimento di Elettronica Applicata
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Meta 2010 & FEM 2010 – Rome, 13-15 December 2010<br />
Role of Resonances of Digital Plasmonic<br />
Gratings in Absorption Profile Remodulation<br />
Pierfrancesco Zilio (1,2) , Davide Sammito (2,3) and Filippo Romanato (1,2,3)<br />
(1) University of Padova, Department of Physics<br />
Padova, Italy – E-mail: pierfrancesco.zilio@pd.infn.it<br />
(2) LaNN - Laboratory of Nanofabriaction of Nanodevices- viale Stati Uniti 4.<br />
35200 Padova, Italy.<br />
(2) IOM-CNR- S.S. 14 km 163.5- Basovizza Trieste<br />
Padova, Italy – E-mail: filippo.romanato@venetonanotech.it<br />
This work investigates the potentialities of 1D subwavelength <strong>di</strong>gital metallic<br />
gratings to modulate the EM field absorption profile in the silicon substrate<br />
underneath. Two well known optical properties of such structures are<br />
particularly attractive for this purpose: Surface Plasmon Polaritons (SPP) and<br />
the Extraor<strong>di</strong>nary Optical Transmission (EOT) [1].<br />
We focused on the optical response of the system to a normally impinging<br />
1000nm-monochromatic TM-polarized wave, varying systematically both<br />
period (d) and thickness (h) of the grating. The ratio between slit width and<br />
period is kept constant to 0.1. The full EM fields <strong>di</strong>stribution has been<br />
computed using COMSOL Multiphysics software which implements a finite<br />
elements analysis. For each configuration (h,d) we calculated transmittance<br />
and absorptance within <strong>di</strong>fferent depths in silicon. We also computed the<br />
effective absorption profile of light as a function of depth in silicon. The same<br />
results have been computed using also a semi-analytical model based on the<br />
decomposition of the fields in Bloch-Floquet modes in air and silicon and in<br />
waveguide modes within the slits [2].<br />
a) b)<br />
Figure 1 – a) Transmittance map as a function of period and thickness of the grating. Solid<br />
lines represent pre<strong>di</strong>ctions of the analytic model. b) Grating configurations showing<br />
respectively Extraor<strong>di</strong>nary Optical Transmission (left) and Surface Plasmon Polaritons (right).<br />
References<br />
[1] F.J. Garcia-Vidal, L.M. Martin-Moreno, T.W. Ebbesen, L. Kuipers, “Light passing<br />
through subwavelength apertures”, Rev. Mod. Phys. , 82, pp. 729-787 (2010).<br />
[2] P. Zilio, D. Sammito, G. Zacco and F. Romanato, “Absorption profile modulation by<br />
means of 1D <strong>di</strong>gital plasmonic gratings”, Optics Express, 18, pp. 19558-19565 (2010).<br />
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