TY - JOUR
T1 - Unraveling unprecedented charge carrier mobility through structure property relationship of four isomers of didodecyl[1]benzothieno[3,2-b][1]benzothiophene
AU - Tsutsui, Yusuke
AU - Schweicher, Guillaume
AU - Chattopadhyay, Basab
AU - Sakurai, Tsuneaki
AU - Arlin, Jean-Baptiste
AU - Ruzié, C.
AU - Aliev, Almaz
AU - Ciesielski, Artur
AU - Colella, Silvia
AU - Kennedy, Alan R.
AU - Lemaur, Vincent
AU - Olivier, Yoann
AU - Hadji, Rachid
AU - Sanguinet, Lionel
AU - Castet, Frédéric
AU - Osella, Silvio
AU - Dudenko, Dymytro
AU - Beljonne, David
AU - Cornil, Jérôme
AU - Samori, Paolo
AU - Seki, Shu
AU - Geerts, Yves H.
PY - 2016/9/7
Y1 - 2016/9/7
N2 - Since the dawn of organic electronics in the 1970’s, academic and industrial research efforts have led to dramatic improvements of the solubility, stability, and electronic properties of organic semiconductors (OSCs).[1, 2] The common benchmark to characterize the electrical performances of OSCs is their charge carrier mobility μ (cm2 V–1 s–1), defined as the drift velocity of the charge carrier (cm s–1) per unit of applied electric field (V cm–1). Reaching high mobilities in OSCs is highly desirable as it allows faster operation of transistors and energy savings by reduced calculation times.[2, 3] However, OSCs performances (conventional values usually range from 1 to 10 cm2 V–1 s–1, with highest values obtained with single-crystal devices mostly exempt of structural defects) are still not comparable to that of state-of-the-art inorganic semiconductors (e.g. metal oxides with µ = 20-50 cm2 V–1 s–1 and polycrystalline silicon with µ > 100 cm2 V–1 s–1) thereby hampering important potential technological applications such as flexible organic light-emitting diode (OLED) displays and wearable electronics.[3, 4]
AB - Since the dawn of organic electronics in the 1970’s, academic and industrial research efforts have led to dramatic improvements of the solubility, stability, and electronic properties of organic semiconductors (OSCs).[1, 2] The common benchmark to characterize the electrical performances of OSCs is their charge carrier mobility μ (cm2 V–1 s–1), defined as the drift velocity of the charge carrier (cm s–1) per unit of applied electric field (V cm–1). Reaching high mobilities in OSCs is highly desirable as it allows faster operation of transistors and energy savings by reduced calculation times.[2, 3] However, OSCs performances (conventional values usually range from 1 to 10 cm2 V–1 s–1, with highest values obtained with single-crystal devices mostly exempt of structural defects) are still not comparable to that of state-of-the-art inorganic semiconductors (e.g. metal oxides with µ = 20-50 cm2 V–1 s–1 and polycrystalline silicon with µ > 100 cm2 V–1 s–1) thereby hampering important potential technological applications such as flexible organic light-emitting diode (OLED) displays and wearable electronics.[3, 4]
KW - organic semiconductors
KW - electrical performances
KW - organic light emitting diodes
UR - http://onlinelibrary.wiley.com/journal/10.1002/%28ISSN%291521-4095
U2 - 10.1002/adma.201601285
DO - 10.1002/adma.201601285
M3 - Article
SN - 1521-4095
VL - 28
SP - 7106
EP - 7114
JO - Advanced Materials
JF - Advanced Materials
IS - 33
ER -