book of abstracts - IM2NP
book of abstracts - IM2NP
book of abstracts - IM2NP
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A B S T R A C T S TUESDAY, JUNE 29 N A N O S E A 2 0 1 0<br />
18H00-18H20<br />
High refractive index modification inside Si02 by femtosecond laser created<br />
self-ordered planar nanostructures.<br />
David Grojo1,2, Thomas Barillot1, Marina Gertsvorlf1,3, Shuting Lei4, David<br />
M. Rayner1 and Paul B. Corkum1,3 (1National Research Council <strong>of</strong> Canada, Steacie Institute for<br />
Molecular Sciences, Ottawa, Canada 2LP3 –UMR 6182, CNRS-Univ. Méditerranée, Marseille, France 3University<br />
<strong>of</strong> Ottawa, Ottawa, Ontario, Canada 4Kansas State University, 2012 Durland Hall, Manhattan, Kansas, USA)<br />
Illumination with intense femtosecond optical pulses focused to small focal spots modifies dielectrics in such<br />
a way that the refractive-index can be locally adjusted. This represents today an attractive micr<strong>of</strong>abrication<br />
method for photonic applications. Here, we investigate the non-uniform nature <strong>of</strong> the strong laser field<br />
ionisation in amorphous silica (a-SiO2) which translates in material cracking at a subwavelength scale.<br />
Under repeated illumination, the cracks migrate to form beautifully-ordered arrays <strong>of</strong> ~8-nm planar<br />
nanocracks with a crack-to-crack spacing <strong>of</strong> λ/2 in the medium. These are extending through the focal region<br />
with no defect and are oriented perpendicular to the laser polarization [1,2]. The material transport is<br />
amazingly driven by the strong laser field making possible to change the writing orientation at anytime with<br />
the polarization. We show the nanotructures are characterized by a very large refractive index change (up to<br />
Δn/n=1.8%) and form birefringence (ns-np ~0.01 at 800 nm). This <strong>of</strong>fers unprecedented control over the<br />
linear optical properties <strong>of</strong> a-SiO2 anywhere in 3-D space. The local change in the focal region leads<br />
progressively to the self-generation <strong>of</strong> a polarization dependent biconvex defocusing microlens (Fig). The<br />
refractive feedback effect on the light that creates the microlens ascribes a self-limited character on the<br />
writing process that is attractive for technological considerations. This is achieved without any noticeable<br />
increase in linear losses and opens a route to adding new functionality inside optical fibers or bulk materials.<br />
[1] V. R. Bhardwaj, E. Simova, P. P. Rajeev, C. Hnatovsky, R. S. Taylor, D. M. Rayner, and P. B. Corkum, Phys. Rev. Lett. 96, (2006)057404<br />
[2] D. Grojo, M. Gertsvolf, H. Jean-Ruel, S. Lei, L. Ramunno, D. M. Rayner, and P. B. Corkum, Appl. Phys. Lett. 93 (2008) 243118.<br />
18H20-18H40<br />
Fabrication <strong>of</strong> an IR emitting ErQ3-based distributed feedback laser by X-ray<br />
Interference Lithography.<br />
S. Prezioso1, P. De Marco1, F. Bisti1, M. Donarelli1, S. Penna2, A. Reale2, S.<br />
Santucci1, and L.Ottaviano1 (1Dipartimento di Fisica, Università dell‟Aquila, gc-LNGS INFN, Via<br />
Vetoio, 67100, L‟Aquila, Italy 2Dip. di Ingegneria Elettronica, Univ. degli studi di Roma “Tor Vergata”, Viale<br />
Politecnico 1, 00133 Roma, Italy)<br />
1 – Introduction<br />
Modern telecommunication technology requires to process large volumes <strong>of</strong> information for scientific,<br />
military and civil purposes. IR light is the most suitable radiation to sustain petabyte-per-year traffics. IR<br />
optical fiber technology is sufficiently mature as well as the micro-electronics industry to accept this<br />
challenge. The bottleneck is represented by the optical interconnection between fiber and chip. The onchip<br />
collection <strong>of</strong> the optical information is one <strong>of</strong> the most promising strategies.<br />
In this work we propose the fabrication <strong>of</strong> an IR emitting ErQ3-based distributed feedback laser as the<br />
onchip light source in charge <strong>of</strong> transferring the information collected from the chip directly into the optical<br />
fiber. Using ErQ3 as the active medium, we can combine the perfect adaptability <strong>of</strong> amorphous organic<br />
materials to any kind <strong>of</strong> surface, periodically modulated surfaces included, with the perfect match <strong>of</strong> Er<br />
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