Jacson de Menezes

Jacson de Menezes

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Research Focus & Metrics

Academic Career Length

21Years (2006-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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3 September 2010 in Advanced Functional Materials
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JMJacson de Menezes
Jacson de Menezes
JFJacqueline Ferreira
Jacqueline Ferreira
MSMarcos J. L. Santos
Marcos J. L. Santos
LCLucila Cescato
Lucila Cescato
ABAlexandre Brolo
Alexandre Brolo

1 January 2006 in Optics Express
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Journal Article
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FQF. Quiñónez
F. Quiñónez
JMJacson de Menezes
Jacson de Menezes
LCL. Cescato
L. Cescato
VEVitaly Felix Rodriguez Esquerre
Vitaly Felix Rodriguez Esquerre
HHH. Hernandez-Figueroa
H. Hernandez-Figueroa
RMR. D. Mansano
R. D. Mansano
Two-dimensional hexagonal photonic crystals can be recorded using the simple superimposition of two interference patterns rotated by 60°. Such process generates high contrast masks, however, it generates elliptical cross section structures instead of cylinders. We study the PBG properties of the experimentally feasible geometries, using this technique and we demonstrate that the effect of this asymmetric shape is a reduction in the PBG map area, for TE polarization, in comparison with cylindrical structures. On the other hand, it appears a PBG for TM polarization.

11 May 2019 in Sensors
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CVChiara Valsecchi
Chiara Valsecchi
LALuis Enrique Armas
Luis Enrique Armas
JMJacson de Menezes
Jacson de Menezes
Several fabrication techniques are recently used to produce a nanopattern for sensing, as focused ion beam milling (FIB), e-beam lithography (EBL), nanoimprinting, and soft lithography. Here, interference lithography is explored for the fabrication of large area nanohole arrays in metal films as an efficient, flexible, and scalable production method. The transmission spectra in air of the 1 cm2 substrate were evaluated to study the substrate behavior when hole-size, periodicity, and film thickness are varied, in order to elucidate the best sample for the most effective sensing performance. The efficiency of the nanohole array was tested for bulk sensing and compared with other platforms found in the literature. The sensitivity of ~1000 nm/RIU, achieved with an array periodicity in the visible range, exceeds near infrared (NIR) performances previously reported, and demonstrates that interference lithography is one of the best alternative to other expensive and time-consuming nanofabrication methods.

1 January 2006 in Optics Express
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JMJacson de Menezes
Jacson de Menezes
LCL. Cescato
L. Cescato
ECE. J. de Carvalho
E. J. de Carvalho
EBE. S. Braga
E. S. Braga
2D hexagonal patterns can be generated by the superimposition of two or three fringe patterns that have been formed by two-wave interference and that have rotations of 60° between them. Superimposing three exposures solves the problem of asymmetry in the cross section of structures, which is caused by double exposure. The resulting structure, however, depends on the phase shift of the third fringe pattern in relation to the previous two. We propose a method for controlling the phase shift, and we demonstrate that three different lattice geometries of hexagonal photonic crystals can be recorded when the phase is chosen.

17 July 2015 in Applied Optics
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JMJacson de Menezes
Jacson de Menezes
ATAnderson Thesing
Anderson Thesing
CVChiara Valsecchi
Chiara Valsecchi
LALuis Enrique Armas
Luis Enrique Armas
ABAlexandre G. Brolo
Alexandre G. Brolo
An experimental investigation on how the bulk and surface sensitivities of gold nanohole arrays fabricated by interference lithography affect the degree of white light beam collimation is presented. The optical transmission response of nanohole arrays has been recorded by focused and collimated beam transmission spectra. The results show that both the bulk and surface sensitivities for the collimated case are much larger than for the focused case. In particular, the shape of the spectra was dependent on the degree of beam collimation. The results showed that improved sensing performance (around 3.5 times) and higher figure of merit (around 4.4 times) can be obtained by simply adjusting the incident/collection experimental conditions in transmission measurements.