Study of the charge transport characteristics of dendrimer molecular thin films

2011 ◽  
Vol 519 (15) ◽  
pp. 5234-5237 ◽  
Author(s):  
J.C. Li ◽  
N. Han ◽  
S.S. Wang ◽  
D.C. Ba
2007 ◽  
Vol 76 (19) ◽  
Author(s):  
M. Sims ◽  
S. M. Tuladhar ◽  
J. Nelson ◽  
R. C. Maher ◽  
M. Campoy-Quiles ◽  
...  
Keyword(s):  

RSC Advances ◽  
2017 ◽  
Vol 7 (86) ◽  
pp. 54911-54919 ◽  
Author(s):  
Varsha Rani ◽  
Akanksha Sharma ◽  
Pramod Kumar ◽  
Budhi Singh ◽  
Subhasis Ghosh

We investigate the charge transport mechanism in copper phthalocyanine thin films with and without traps. We find that the density of interface states at the grain boundaries can decide the mechanism of charge transport in organic thin films.


2001 ◽  
Vol 388 (1-2) ◽  
pp. 171-176 ◽  
Author(s):  
R. Valaski ◽  
S. Ayoub ◽  
L. Micaroni ◽  
I.A. Hümmelgen

2009 ◽  
Vol 21 (16) ◽  
pp. NA-NA
Author(s):  
Leslie H. Jimison ◽  
Michael F. Toney ◽  
Iain McCulloch ◽  
Martin Heeney ◽  
Alberto Salleo

Langmuir ◽  
2016 ◽  
Vol 32 (42) ◽  
pp. 10851-10860 ◽  
Author(s):  
Naisheng Jiang ◽  
Levent Sendogdular ◽  
Mani Sen ◽  
Maya K. Endoh ◽  
Tadanori Koga ◽  
...  

Polymers ◽  
2020 ◽  
Vol 12 (5) ◽  
pp. 1188
Author(s):  
Mingu Jang ◽  
Yang-Il Huh ◽  
Mincheol Chang

We systematically studied the influence of solvent vapor annealing on the molecular ordering, morphologies, and charge transport properties of poly(3-hexylthiophene) (P3HT) thin films embedded with preformed crystalline P3HT nanowires (NWs). Solvent vapor annealing (SVA) with chloroform (CF) was found to profoundly impact on the structural and morphological changes, and thus on the charge transport characteristics, of the P3HT-NW-embedded P3HT films. With increased annealing time, the density of crystalline P3HT NWs was increased within the resultant films, and also intra- and intermolecular interactions of the corresponding films were significantly improved. As a result, the P3HT-NW-embedded P3HT films annealed with CF vapor for 20 min resulted in a maximized charge carrier mobility of ~0.102 cm2 V−1 s−1, which is higher than that of pristine P3HT films by 4.4-fold (μ = ~0.023 cm2 V−1 s−1).


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