Pyrene-Incorporated Side Chain in π-Conjugated Polymers for Non-Volatile Transistor-Type Memory Devices with Improved Stretchability

2021 ◽  
Vol 3 (4) ◽  
pp. 2109-2119
Author(s):  
Yan-Cheng Lin ◽  
Chih-Chien Hung ◽  
Chun-Kai Chen ◽  
Yun-Chi Chiang ◽  
Li-Che Hsu ◽  
...  
2012 ◽  
Vol 22 (19) ◽  
pp. 9576 ◽  
Author(s):  
Peng Wang ◽  
Shu-Juan Liu ◽  
Zhen-Hua Lin ◽  
Xiao-Chen Dong ◽  
Qiang Zhao ◽  
...  

2012 ◽  
Vol 22 (43) ◽  
pp. 22964 ◽  
Author(s):  
Shu-Juan Liu ◽  
Wen-Peng Lin ◽  
Ming-Dong Yi ◽  
Wen-Juan Xu ◽  
Chao Tang ◽  
...  

Author(s):  
Guitao Feng ◽  
Wenliang Tan ◽  
Safakath Karuthedath ◽  
Cheng Li ◽  
Xuechen Jiao ◽  
...  

2018 ◽  
Vol 30 (3) ◽  
pp. 2235-2245
Author(s):  
Wenjie Deng ◽  
Yuancheng Qin ◽  
Shanshan Lin ◽  
Dezhong Song ◽  
Sha Xu ◽  
...  

2018 ◽  
Vol 30 (9) ◽  
pp. 2945-2953 ◽  
Author(s):  
Alexander Giovannitti ◽  
Iuliana P. Maria ◽  
David Hanifi ◽  
Mary J. Donahue ◽  
Daniel Bryant ◽  
...  

2016 ◽  
Vol 7 (1) ◽  
pp. 101-112 ◽  
Author(s):  
Ana Fokina ◽  
Yeonkyung Lee ◽  
Jun Hyuk Chang ◽  
Lydia Braun ◽  
Wan Ki Bae ◽  
...  

Three monomers,M1–M3, with modified carbazole cores and styrene functionality were polymerized by RAFT. The polymers were then used in the active layers of hybrid polymer/quantum dot light emitting diodes.


2018 ◽  
Vol 51 (7) ◽  
pp. 2580-2590 ◽  
Author(s):  
Brenden McDearmon ◽  
Eunhee Lim ◽  
In-Hwan Lee ◽  
Lisa M. Kozycz ◽  
Kathryn O’Hara ◽  
...  

Polymers ◽  
2020 ◽  
Vol 12 (6) ◽  
pp. 1207
Author(s):  
Quoc-Trung Vu ◽  
Thi-Thuy-Duong Tran ◽  
Thuy-Chinh Nguyen ◽  
Thien Vuong Nguyen ◽  
Hien Nguyen ◽  
...  

Conjugated polymers are promising materials for various cutting-edge technologies, especially for organic conducting materials and in the energy field. In this work, we have synthesized a new conjugated polymer and investigated the effect of distance between bond layers, side-chain functional groups (H, Br, OH, OCH3 and OC2H5) on structural characteristics, phase transition temperature (T), and electrical structure of C13H8OS using Density Functional Theory (DFT). The structural characteristics were determined by the shape, network constant (a, b and c), bond length (C–C, C–H, C–O, C–S, C–Br and O–H), phase transition temperatures, and the total energy (Etot) on a base cell. Our finding shows that the increase of layer thickness (h) of C13H8OS–H has a negligible effect on the transition temperature, while the energy bandgap (Eg) increases from 1.646 eV to 1.675 eV. The calculation of bond length with different side chain groups was carried out for which C13H8OS–H has C–H = 1.09 Å; C13H8OS–Br has C–Br = 1.93 Å; C13H8OS–OH has C–O = 1.36 Å, O–H = 0.78 Å; C13H8OS–OCH3 has C–O = 1.44 Å, O–H =1.10 Å; C13H8OS–OC2H5 has C–O = 1.45 Å, C–C = 1.51Å, C–H = 1.10 Å. The transition temperature (T) for C13H8OS–H was 500 K < T < 562 K; C13H8OS–Br was 442 K < T < 512 K; C13H8OS–OH was 487 K < T < 543 K; C13H8OS–OCH3 was 492 K < T < 558 K; and C13H8OS–OC2H5 was 492 K < T < 572 K. The energy bandgap (Eg) of Br is of Eg = 1.621 eV, the doping of side chain groups H, OH, OCH3, and OC2H5, leads to an increase of Eg from 1.621 eV to 1.646, 1.697, 1.920, and 2.04 eV, respectively.


2019 ◽  
Vol 10 (47) ◽  
pp. 6473-6480 ◽  
Author(s):  
Ruimin Diao ◽  
Haonan Ye ◽  
Zhicheng Yang ◽  
Shicong Zhang ◽  
Kangyi Kong ◽  
...  

The hydrogen evolution rate of PDPP3B-O4 with butoxy chain was 5.53 mmol h−1 g−1 with 1% Pt loading (λ > 400 nm), increased 110 times than PDPP3B-C8 with octyl chain due to wider absorption spectrum and better wettability via side chain engineering.


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