Optically active helical structure and magnetic interaction of poly(phenylacetylene)-based polyradicals

Polyhedron ◽  
2009 ◽  
Vol 28 (9-10) ◽  
pp. 1927-1929 ◽  
Author(s):  
Takashi Kaneko ◽  
Hiroo Katagiri ◽  
Yasuhiro Umeda ◽  
Takeshi Namikoshi ◽  
Edy Marwanta ◽  
...  
1989 ◽  
Vol 175 ◽  
Author(s):  
S.H. Chen ◽  
M.L. Tsai ◽  
S.D. Jacobs

AbstractChiral nematic copolymers based on optically active cholesterol, dihydrocholesterol, (R)-(+)- and (S)-(−)-1-phenylethylamine, and (+)- and (−)- isopinocampheol were synthesized and characterized for the investigations of thermotropic and optical properties. Although helical sense does not appear to correlate with the sign of [α]D of the precursor chiral compound as suggested by the observations of cholesteryl and dihydrocholesteryl copolymers, the inversion of chirality in the pendant group, (R)-(+)- vs (S)-(−)-1-phenylethylamine, does lead to the opposite handedness in the resultant helical structure. To better understand the structure-property relationships involving helical sense and twisting power, systematic studies of the roles played by both nematogenic and chiral structures as well as other structural features of the comonomers should be conducted.


2006 ◽  
Vol 39 (9) ◽  
pp. 3103-3105 ◽  
Author(s):  
Toshiyuki Fukushima ◽  
Kiyohiro Takachi ◽  
Kenji Tsuchihara

2014 ◽  
Vol 92 (7) ◽  
pp. 647-652
Author(s):  
Yehui Chen ◽  
Liwen Yang ◽  
Nianfa Yang ◽  
Zhusheng Yang

(S)-3-acrylyl-2,2′-bis(methoxymethoxy)-1,1′-binaphthyl (3a) was synthesized and anionically polymerized using n-BuLi as an initiator. The polymer derived from 3a had a tremendous specific optical rotation [Formula: see text] = −304.2, while that of the monomer 3a is −68.7. Poly-3a was confirmed to exist in the form of a one-handed helical structure in solution by means of comparing the specific optical rotation, the circular dichroism, and UV-vis spectra with that of 3a and the model compounds such as (S)-3-propionyl-2,2′-bis(methoxymethoxy)-1,1′-binaphthyl (3b) and (S)-3-heptanoyl-2,2′-bis(methoxymethoxy)-1,1′-binaphthyl (3c). This conclusion was also confirmed by the fact that the g value of poly-3a is about 15 times of that of the monomer 3a.


2015 ◽  
Vol 66 (1) ◽  
pp. 57-60
Author(s):  
Dániel Datz ◽  
Antal Gasparics ◽  
Gábor Vértesy

Abstract Markers for imaging are vital parts of surgical processes. Since radioactive compound pose considerable risk to both the recipient and the surgical staff, alternative marking techniques are of interest. In NANOMAGDYE project, magneto-optically active nano-particles were created for this reason. The detection of the magnetic interaction of low mass nano-particles in surgical environment is very challenging; so far only quasi-stationary measurements were taken. This paper shows a measurement setup for measurements with continuously moving probe at lower velocities (5–10 mm/s) and at hand movement velocity (20–30 cm/s). It was found that at the velocity of hand movement there is only probe response amplitude reduction of at most 10–15% of the original amplitude. These results indicate that the probe used for the detection of the nano-particles is sufficient to be used in practical purposes in surgery.


e-Polymers ◽  
2012 ◽  
Vol 12 (1) ◽  
Author(s):  
Lihua Lu ◽  
Jiaoli Mo ◽  
Qiang Yang ◽  
Liqun Zhang ◽  
Weimin Wang ◽  
...  

AbstractNovel chiral and achiral N-propargylphosphonamidate monomers [HC=CCH2NH(P=O)R1R2,where 1: R1=CH3,R2=NHC(CH3)32: R1=CH3,R2 =NHC5H93:R1=OPh,R2=NHC(CH3)3, 4:R1=R2=OPh] were synthesized by successive condensation in order to study the helical conformation properties of N-phosphonamidates. One diastereomer was successfully separated from the other in the cases of monomer 1-3(named 1a-3a) according to the single peak in the 31P NMR spectra. Polymerizations of the monomers 1-4 were carried out with (nbd)Rh+[η6-C6H5B-(C6H5)3] as catalyst in CHCl3 yielding the polymers with number-average molecular weights of 1300-22400. Poly(1a)-poly(3a) and poly(4) were characterized by UV and CD spectroscopy. Poly(1a)- poly(3a) showed an intense positive CD signal at 325 nm based on the conjugated polyacetylene backbone while poly(4) showed no peak there, indicating that the polymers had a helical structure with predominantly one-handed screw sense because of P-chiral centre sole contribution.


2020 ◽  
Vol 11 (39) ◽  
pp. 6241-6250
Author(s):  
Naoya Kanbayashi ◽  
Marina Saegusa ◽  
Yuki Ishido ◽  
Taka-aki Okamura ◽  
Kiyotaka Onitsuka

Herein we present the precise design and synthesis of a novel polymer backbone that induces a helical structure through asymmetric polymerization reactions of a phthalimide-based monomer catalyzed by a planar-chiral cyclopentadienyl–ruthenium complex.


Author(s):  
George C. Ruben ◽  
William Krakow

Tobacco primary cell wall and normal bacterial Acetobacter xylinum cellulose formation produced a 36.8±3Å triple-stranded left-hand helical microfibril in freeze-dried Pt-C replicas and in negatively stained preparations for TEM. As three submicrofibril strands exit the wall of Axylinum , they twist together to form a left-hand helical microfibril. This process is driven by the left-hand helical structure of the submicrofibril and by cellulose synthesis. That is, as the submicrofibril is elongating at the wall, it is also being left-hand twisted and twisted together with two other submicrofibrils. The submicrofibril appears to have the dimensions of a nine (l-4)-ß-D-glucan parallel chain crystalline unit whose long, 23Å, and short, 19Å, diagonals form major and minor left-handed axial surface ridges every 36Å.The computer generated optical diffraction of this model and its corresponding image have been compared. The submicrofibril model was used to construct a microfibril model. This model and corresponding microfibril images have also been optically diffracted and comparedIn this paper we compare two less complex microfibril models. The first model (Fig. 1a) is constructed with cylindrical submicrofibrils. The second model (Fig. 2a) is also constructed with three submicrofibrils but with a single 23 Å diagonal, projecting from a rounded cross section and left-hand helically twisted, with a 36Å repeat, similar to the original model (45°±10° crossover angle). The submicrofibrils cross the microfibril axis at roughly a 45°±10° angle, the same crossover angle observed in microflbril TEM images. These models were constructed so that the maximum diameter of the submicrofibrils was 23Å and the overall microfibril diameters were similar to Pt-C coated image diameters of ∼50Å and not the actual diameter of 36.5Å. The methods for computing optical diffraction patterns have been published before.


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