TY - JOUR
T1 - Parylene-C microfibrous thin films as phononic crystals
AU - Chindam, Chandraprakash
AU - Lakhtakia, Akhlesh
AU - Awadelkarim, Osama O.
N1 - Funding Information:
We thank the Research and Cyberinfrastructure Center of Institute of Cyber Science (ICS) of the Pennsylvania State University for computing resources, Brian Van Leeuwen and Hirofumi Akamatsu of the Department of Materials Science and Engineering (Penn State) for help in identifying irreducible Brillouin zones, and Anand Kumar Singh (ICS) and Chien Liu (COMSOL support team) for assistance with meshrelated issues.
Publisher Copyright:
© 2017 IOP Publishing Ltd.
Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.
PY - 2017/6/6
Y1 - 2017/6/6
N2 - Phononic bandgaps of Parylene-C microfibrous thin films (μFTFs) were computationally determined by treating them as phononic crystals comprising identical microfibers arranged either on a square or a hexagonal lattice. The microfibers could be columnar, chevronic, or helical in shape, and the host medium could be either water or air. All bandgaps were observed to lie in the 0.01-162.9-MHz regime, for microfibers of realistically chosen dimensions. The upper limit of the frequency of bandgaps was the highest for the columnar μFTF and the lowest for the chiral μFTF. More bandgaps exist when the host medium is water than air. Complete bandgaps were observed for the columnar μFTF with microfibers arranged on a hexagonal lattice in air, the chevronic μFTF with microfibers arranged on a square lattice in water, and the chiral μFTF with microfibers arranged on a hexagonal lattice in either air or water. The softness of the Parylene-C μFTFs makes them mechanically tunable, and their bandgaps can be exploited in multiband ultrasonic filters.
AB - Phononic bandgaps of Parylene-C microfibrous thin films (μFTFs) were computationally determined by treating them as phononic crystals comprising identical microfibers arranged either on a square or a hexagonal lattice. The microfibers could be columnar, chevronic, or helical in shape, and the host medium could be either water or air. All bandgaps were observed to lie in the 0.01-162.9-MHz regime, for microfibers of realistically chosen dimensions. The upper limit of the frequency of bandgaps was the highest for the columnar μFTF and the lowest for the chiral μFTF. More bandgaps exist when the host medium is water than air. Complete bandgaps were observed for the columnar μFTF with microfibers arranged on a hexagonal lattice in air, the chevronic μFTF with microfibers arranged on a square lattice in water, and the chiral μFTF with microfibers arranged on a hexagonal lattice in either air or water. The softness of the Parylene-C μFTFs makes them mechanically tunable, and their bandgaps can be exploited in multiband ultrasonic filters.
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U2 - 10.1088/1361-6439/aa717f
DO - 10.1088/1361-6439/aa717f
M3 - Article
AN - SCOPUS:85021348356
VL - 27
JO - Journal of Micromechanics and Microengineering
JF - Journal of Micromechanics and Microengineering
SN - 0960-1317
IS - 7
M1 - 075012
ER -