106620-89-7

Upstream product

• 79-41-4 poly(methacrylic acid) 
• 59100-59-3 4-(11'-hydroxyundecyloxy)benzoic acid 
• 920-46-7 Methacryloyl chloride 
• 1611-56-9 1-Bromo-11-hydroxyundecane 
• 99-96-7 4-hydroxy-benzoic acid 
• 94-18-8 Benzyl 4-hydroxybenzoate 
• 724449-03-0 benzyl 4-(11'-hydroxyundecyloxy)benzoate 

Downstream Products

• 836608-59-4 (S)-2-methylbutyl 7-[4-(11-methacryloyloxyundecyloxy)benzoyloxy]-2-oxo-2H-1-benzopyran-3-carboxylate 
• 951170-95-9 4-(11-methacryloyloxyundecyloxy)benzoic 4-butylbenzamide 
• 184171-56-0 2-Methyl-acrylic acid 11-(4-chlorocarbonyl-phenoxy)-undecyl ester 

Relevant academic research and scientific papers

METAL COMPLEX, COMPOSITION COMPRISING SAME AND LIGHT-EMITTING ELEMENT USING SAME

The invention provides a metal complex having a structure represented by the following formula (1): wherein M represents a metal atom such as copper; C1 and C2 are each an sp3 carbon atom; A1-A4 each independent

Stable macroscopic nanocylinder arrays in an amphiphilic diblock liquid-crystalline copolymer with successive hydrogen bonds

In bulk films of a novel well-defined amphiphilic diblock liquid-crystalline copolymer with aramid moieties, a stable perpendicularly orientated hydrophilic nanocylinder array with hexagonal packing was formed in a large area by supramolecular self-assemb

SmCP-Networked films obtained by in situ photopolymerization of neat reactive banana-shaped liquid crystals

The synthesis and characterization of reactive banana-shaped compounds have been carried out, and their ability to be photopolymerized in their SmCP mesophase has been assessed. The presence of a SmCP liquid crystalline phase in these compounds has been c

SYNTHESIS AND THERMAL PROPERTIES OF SIDE CHAIN TYPE LIQUID CRYSTALLINE POLYMERS WITH CHIRAL UNIT IN THE FLEXIBLE MOIETY

This paper is concerned with the synthesis and thermal properties for five families of side-chain type liquid crystalline polymers.All these side-chain type polymers showed an enantiotropic mesomorphic nature.A sharp reflexion was observed in the small angle region, whereas a broad halo or a relatively sharp peak was also detected in the wide angle region for all the polymers.The experimental values of the thickness of the smectic layer which can be easily assigned by the polarizing microscopic measurements were smaller than that of the calculated ones.This difference would be caused from the tilted arrangement in the smectic layer or smectic A like structure in which the side chain would be overlapped.