Synthesis of tailored core–brush polymer particles via a living radical polymerization and architecture of colloidal crystals

Synthesis of core–shell polymer particle. [Display omitted] ► Core–brush polymer particles (BP) were prepared by grafting from a photo-induced ATRP with 2-hydroxyethyl methacrylate (HEMA) initiated by photo-functional polymer particles (EP) having N, N-diethyldithiocarbamate (DC) groups at surface....

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Published inJournal of Colloid and Interface Science Vol. 353; no. 1; pp. 69 - 75
Main Authors Ishizu, Koji, Amir, Isamu, Okamoto, Nobuyuki, Uchida, Satoshi, Ozawa, Masaaki, Chen, Hui
Format Journal Article
LanguageEnglish
Published Amsterdam Elsevier Inc 2011
Elsevier BV
Elsevier
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ISSN0021-9797
1095-7103
1095-7103
DOI10.1016/j.jcis.2010.08.067

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Summary:Synthesis of core–shell polymer particle. [Display omitted] ► Core–brush polymer particles (BP) were prepared by grafting from a photo-induced ATRP with 2-hydroxyethyl methacrylate (HEMA) initiated by photo-functional polymer particles (EP) having N, N-diethyldithiocarbamate (DC) groups at surface. ► We constructed colloidal crystals (CC) of BP and locked CC by cross-linking of PHEMA brush phases with glutaraldehyde. ► The peak wavelength (λ max) in the reflection spectra agreed well with the bandgap position for light incident on the (1 1 1) face of face-centered cubic (fcc) lattice according to Bragg’s law. Narrow disperse core–brush polymer nanoparticles (BP) were synthesized by grafting from photo-induced atom transfer radical polymerization (ATRP) of 2-hydroxyethyl methacrylate (HEMA) from N, N-diethyldithiocarbamate (DC) groups of core–shell particle surface. We constructed colloidal crystals of these particles by depositing on glass substrate. By variation of the particle size, the brilliant color could be varied throughout the visible spectrum. We locked also permanently such colloidal crystals by cross-linking of poly(2-hydroxyethyl methacrylate) (PHEMA) brush phases with glutaraldehyde. The peak wavelength ( λ max) in the reflection spectra agreed well with the bandgap position for light incident on the (1 1 1) face of face-centered cubic (fcc) lattice according to Bragg’s law.
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ISSN:0021-9797
1095-7103
1095-7103
DOI:10.1016/j.jcis.2010.08.067