2010
DOI: 10.1109/lpt.2010.2048310
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Fabrication of a Polymeric Optical Waveguide-On-Flex Using Electrostatic-Induced Lithography

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Cited by 7 publications
(6 citation statements)
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“…As a direct consequence, the excess charges continuously produced during the heating process and distributed according to the domain structures, are no longer attracted by the polarization charge and, consequently, they result free to diffuse into the liquid. The electric forces at the solid-liquid interface are responsible of the polymer shaping, in particular in this case, the force acting on the polymeric film and produced by the pyro-EHD effect can be deduced by the Maxwell stress tensor [30]:…”
Section: Fabrication Processmentioning
confidence: 99%
“…As a direct consequence, the excess charges continuously produced during the heating process and distributed according to the domain structures, are no longer attracted by the polarization charge and, consequently, they result free to diffuse into the liquid. The electric forces at the solid-liquid interface are responsible of the polymer shaping, in particular in this case, the force acting on the polymeric film and produced by the pyro-EHD effect can be deduced by the Maxwell stress tensor [30]:…”
Section: Fabrication Processmentioning
confidence: 99%
“…In this patterning technique, a thin polymer film deforms and self-assembles into micro and nanostructures under either a featureless mask or patterned mask subject to a high electrostatic voltage. The successful replication of sub-micron periodic grating structures in polymer has been demonstrated by this method [3,4]. Figure 1 shows the experimental setup used in this patterning technique.…”
Section: Introductionmentioning
confidence: 99%
“…The underlying physical phenomenon responsible for this technique, the instability of polymer lms on planar substrates when exposed to an external electric eld, has also been intensively researched from the theoretical and experimental points of view, and structures including columns, ridges, holes, channels and even hollow structures have been demonstrated. [9][10][11][12][13][14][15][16][17][18][19][20][21][22] However, the stability of a thin lm on a curved surface is rather different from the planar one. For the case of the at surface, the electric eld overcomes the in-plane curvature to engender structures like columns, holes, or channels on the lm.…”
Section: Introductionmentioning
confidence: 99%