Literature DB >> 25544779

Influence of non-reactive solvent on optical performance, photopolymerization kinetics and morphology of nanoporous polymer gratings.

Vincent K S Hsiao1, Timothy J White2, Alexander N Cartwright3, Paras N Prasad4, C Allan Guymon2.   

Abstract

A study of nanoporous polymer gratings, with controllable nanostructured porosity, as a function of grating performance, photopolymerization kinetics and morphology is presented. Modifying the standard holographic polymer dispersed liquid crystal (H-PDLC) system, by including a non-reactive solvent, results in a layered, nanoporous morphology and produces reflective optical elements with excellent optical performance of broadband reflection. The addition of the non-reactive solvent in the pre-polymer mixture results in a morphology typified by void/polymer layer-by-layer structures if sufficient optical energy is used during the holographic writing process. The duration and intensity of optical exposure necessary to form well-aligned nanoporous structures can only be obtained in the modified system by (a) illumination under longer time of holographic interference patterning (30 min) or (b) illumination under very short time of holographic interference patterning (30 s) and followed by post-curing using homogeneous optical exposure for 60 min. Comparatively, a typical H-PDLC is formed in less than 1 min. To further understand the differences in the formation of these two analogous materials, the temporal dynamics of the photoinitiation and polymerization (propagation) kinetics were examined. It is shown herein that the writing exposure gives a cross-linked polymer network that is denser in the bright regions. With 60% (or even 45%) acrylate conversion, almost no free monomer would be left after the writing. Continued exposure serves primarily to add cross-links. This has the tendency to collapse the network, especially the less dense portions, which in effect get glued down to the more dense parts. To the extent that the solvent increases the mobility of the polymer network, this process will be aided. Equally important, the size of the periodic nanopores can be varied from 10 to 50 nm by controlling either the LC concentration in the pre-polymer mixture or by controlling the time of the homogeneous post-cure.

Entities:  

Keywords:  Holographic polymer dispersed liquid crystal; Nanoporous polymer; Phase separation; Photopolymerization kinetics

Year:  2010        PMID: 25544779      PMCID: PMC4276335          DOI: 10.1016/j.eurpolymj.2010.01.022

Source DB:  PubMed          Journal:  Eur Polym J        ISSN: 0014-3057            Impact factor:   4.598


  3 in total

1.  Switchable orthorhombic F photonic crystals formed by holographic polymerization-induced phase separation of liquid crystal.

Authors:  Richard Sutherland; V Tondiglia; L Natarajan; S Chandra; D Tomlin; T Bunning
Journal:  Opt Express       Date:  2002-10-07       Impact factor: 3.894

2.  Nanoporous polymeric transmission gratings for high-speed humidity sensing.

Authors:  Jinjie Shi; Vincent K S Hsiao; Tony Jun Huang
Journal:  Nanotechnology       Date:  2007-10-12       Impact factor: 3.874

3.  High contrast switching of distributed-feedback lasing in dye-doped H-PDLC transmission grating structures.

Authors:  Vincent Hsiao; Changgui Lu; Guang He; Michael Pan; Alexander Cartwright; Paras Prasad; Rachel Jakubiak; Richard Vaia; Timothy Bunning
Journal:  Opt Express       Date:  2005-05-16       Impact factor: 3.894

  3 in total
  1 in total

1.  Holographic photopolymer linear variable filter with enhanced blue reflection.

Authors:  Tania Moein; Dengxin Ji; Xie Zeng; Ke Liu; Qiaoqiang Gan; Alexander N Cartwright
Journal:  ACS Appl Mater Interfaces       Date:  2014-02-18       Impact factor: 9.229

  1 in total

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