Effect of process parameters on sidewall roughness in polymeric optical waveguides

2004 ◽  
Vol 462-463 ◽  
pp. 471-476 ◽  
Author(s):  
S.K. Pani ◽  
C.C. Wong ◽  
K. Sudharsanam ◽  
S.G. Mhaisalkar ◽  
V. Lim ◽  
...  
2013 ◽  
Vol 5 (3) ◽  
pp. 6601010-6601010 ◽  
Author(s):  
E. Jaberansary ◽  
T. M. B. Masaud ◽  
M. M. Milosevic ◽  
M. Nedeljkovic ◽  
G. Z. Mashanovich ◽  
...  

2010 ◽  
Vol 28 (10) ◽  
pp. 1510-1520 ◽  
Author(s):  
Andrea Di Donato ◽  
Marco Farina ◽  
Davide Mencarelli ◽  
Agnese Lucesoli ◽  
Silvia Fabiani ◽  
...  

2006 ◽  
Vol 6 (11) ◽  
pp. 3562-3566
Author(s):  
W. S. Choi ◽  
J. H. Jang ◽  
B.-A. Yu ◽  
Y. L. Lee ◽  
W. Zhao ◽  
...  

Low loss high mesa optical waveguides were fabricated on InGaAsP/InP heterostructures by utilizing inductively-coupled-plasma reactive ion etching (ICP-RIE) and electron beam lithography technique. The fabrication process was optimized by measuring sidewall roughness of deep-etched waveguides. Atomic force microscope loaded with carbon nanotude was used to obtain three-dimensional image of the etched sidewall of waveguides. The obtained statistical information such as rms roughness and correlation length was used to theoretically calculate scattering loss of waveguides. Several waveguides with different number of sharp bends and the length were fabricated and their propagation losses were measured by modified Fabry-Perot method. The measured propagation losses were compared with theoretically calculated losses.


2005 ◽  
Vol 239 (3-4) ◽  
pp. 445-450 ◽  
Author(s):  
S.K. Pani ◽  
C.C. Wong ◽  
K. Sudharsanam ◽  
V. Lim

2003 ◽  
Vol 83 (20) ◽  
pp. 4116-4118 ◽  
Author(s):  
J. H. Jang ◽  
W. Zhao ◽  
J. W. Bae ◽  
D. Selvanathan ◽  
S. L. Rommel ◽  
...  

Author(s):  
W. E. Lee

An optical waveguide consists of a several-micron wide channel with a slightly different index of refraction than the host substrate; light can be trapped in the channel by total internal reflection.Optical waveguides can be formed from single-crystal LiNbO3 using the proton exhange technique. In this technique, polished specimens are masked with polycrystal1ine chromium in such a way as to leave 3-13 μm wide channels. These are held in benzoic acid at 249°C for 5 minutes allowing protons to exchange for lithium ions within the channels causing an increase in the refractive index of the channel and creating the waveguide. Unfortunately, optical measurements often reveal a loss in waveguiding ability up to several weeks after exchange.


1985 ◽  
Vol 132 (6) ◽  
pp. 314 ◽  
Author(s):  
J.M. Arnold ◽  
A. Belghoraf ◽  
A. Dendane

2020 ◽  
Vol 90 (3) ◽  
pp. 30502
Author(s):  
Alessandro Fantoni ◽  
João Costa ◽  
Paulo Lourenço ◽  
Manuela Vieira

Amorphous silicon PECVD photonic integrated devices are promising candidates for low cost sensing applications. This manuscript reports a simulation analysis about the impact on the overall efficiency caused by the lithography imperfections in the deposition process. The tolerance to the fabrication defects of a photonic sensor based on surface plasmonic resonance is analysed. The simulations are performed with FDTD and BPM algorithms. The device is a plasmonic interferometer composed by an a-Si:H waveguide covered by a thin gold layer. The sensing analysis is performed by equally splitting the input light into two arms, allowing the sensor to be calibrated by its reference arm. Two different 1 × 2 power splitter configurations are presented: a directional coupler and a multimode interference splitter. The waveguide sidewall roughness is considered as the major negative effect caused by deposition imperfections. The simulation results show that plasmonic effects can be excited in the interferometric waveguide structure, allowing a sensing device with enough sensitivity to support the functioning of a bio sensor for high throughput screening. In addition, the good tolerance to the waveguide wall roughness, points out the PECVD deposition technique as reliable method for the overall sensor system to be produced in a low-cost system. The large area deposition of photonics structures, allowed by the PECVD method, can be explored to design a multiplexed system for analysis of multiple biomarkers to further increase the tolerance to fabrication defects.


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