Hole Mobilities in Trivalent Metal Phthalocyanine Thin Films. 1. Activated Charge Transport in Time-of-Flight Measurements between 333 and 213 K for Chloroaluminum Phthalocyanine Films with Various Amounts of Disorder

1997 ◽  
Vol 101 (6) ◽  
pp. 891-900 ◽  
Author(s):  
A. Ioannidis ◽  
J. P. Dodelet
Keyword(s):  
Thin Films ◽  
Charge Transport ◽  
Time Of Flight ◽  
Metal Phthalocyanine ◽  
Trivalent Metal ◽  
Chloroaluminum Phthalocyanine ◽  
Flight Measurements

Charge transport in poly(3-hexylthiophene):CdSe nanocrystals hybrid thin films investigated with time-of-flight measurements

2012 ◽  
Vol 101 (13) ◽  
pp. 133301 ◽  
Author(s):  
Elsa Couderc ◽  
Nicolas Bruyant ◽  
Angela Fiore ◽  
Frédéric Chandezon ◽  
David Djurado ◽  
...  
Keyword(s):  
Thin Films ◽  
Charge Transport ◽  
Time Of Flight ◽  
Cdse Nanocrystals ◽  
Hybrid Thin Films ◽  
Flight Measurements

Time-of-flight measurements in thin films of regioregular poly(3-hexyl thiophene)

2000 ◽  
Vol 109 (1-3) ◽  
pp. 173-176 ◽  
Author(s):  
G. Juska ◽  
K. Arlauskas ◽  
R. Österbacka ◽  
H. Stubb
Keyword(s):  
Thin Films ◽  
Time Of Flight ◽  
Regioregular Poly ◽  
Flight Measurements

Time-of-flight study of electrical charge mobilities in liquid-crystalline zinc octakis(β-octoxyethyl) porphyrin films

2000 ◽  
Vol 15 (11) ◽  
pp. 2494-2498 ◽  
Author(s):  
Yang Yuan ◽  
Brian A. Gregg ◽  
Marcus F. Lawrence
Keyword(s):  
Charge Transport ◽  
Liquid Crystalline ◽  
Room Temperature ◽  
Thick Films ◽  
Time Of Flight ◽  
Charge Carriers ◽  
Electrical Charge ◽  
Charged Carrier ◽  
Flight Measurements ◽  
Discotic Mesophase

Time-of-flight measurements performed on micron-thick films of liquid-crystalline zinc octakis(β-octoxyethyl) porphyrin indicated that charge carriers possess significantly high drift mobilities, attaining approximately 0.01 cm2 V−1s −1 and 0.008 cm2 V−1s −1 for holes and electrons, respectively, at room temperature. Upon heating the samples from 300 to 420 K, causing the porphyrin to go from the solid-crystalline to the discotic mesophase, the mobilities did not decrease drastically, and remained at values slightly larger than half those observed at room temperature. Charge transport in this material conformed to the Scher–Montroll model, which attributes a distribution of hopping times to the propagation of the initially formed charged carrier packet. Analysis of the “universal” plots prescribed by this model yielded a dispersion factor of 0.5 for both charge carriers.

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