TY - JOUR
T1 - Improving efficiency by balancing carrier transport in poly(9,9-dioctylfluorene) light-emitting diodes using tetraphenylporphyrin as a hole-trapping, emissive dopant
AU - Campbell, Alasdair J.
AU - Bradley, Donal D.C.
AU - Virgili, Tersilla
AU - Lidzey, David G.
AU - Antoniadis, Homer
N1 - Generated from Scopus record by KAUST IRTS on 2019-11-27
PY - 2001/12/3
Y1 - 2001/12/3
N2 - Unbalanced carrier transport is known to strongly affect the efficiency of polymer light-emitting diodes. Here, we report the results of time-of-flight (TOF), current density-voltage, and electroluminescence (EL) quantum efficiency measurements on single-layer poly(9,9-dioctylfluorene) (PFO) devices doped with the red-emitter tetraphenylporphyrin (TPP). TOF shows that PFO is a unipolar conductor, with hole transport much better than electron transport. At a field of 5 × 105 V/cm, a nondispersive hole mobility of 4 × 10-5-5 × 10-4 cm2/V s, dependent on sample morphology, is obtained. Upon the addition of 5% by weight TPP, hole transport becomes as highly dispersive as electron transport, having no measurable average mobility. This results in a decrease in the current for a given applied bias but an increase in the external EL quantum efficiency. TPP acts as a strong hole trap, reducing the dominant hole current and producing more balanced carrier transport. At TPP concentrations above 6%, the device characteristics start to revert to those found at lower TPP concentrations. This is due to the onset of efficient hole transport between the dopant molecules that reestablishes a transport imbalance. © 2001 American Institute of Physics.
AB - Unbalanced carrier transport is known to strongly affect the efficiency of polymer light-emitting diodes. Here, we report the results of time-of-flight (TOF), current density-voltage, and electroluminescence (EL) quantum efficiency measurements on single-layer poly(9,9-dioctylfluorene) (PFO) devices doped with the red-emitter tetraphenylporphyrin (TPP). TOF shows that PFO is a unipolar conductor, with hole transport much better than electron transport. At a field of 5 × 105 V/cm, a nondispersive hole mobility of 4 × 10-5-5 × 10-4 cm2/V s, dependent on sample morphology, is obtained. Upon the addition of 5% by weight TPP, hole transport becomes as highly dispersive as electron transport, having no measurable average mobility. This results in a decrease in the current for a given applied bias but an increase in the external EL quantum efficiency. TPP acts as a strong hole trap, reducing the dominant hole current and producing more balanced carrier transport. At TPP concentrations above 6%, the device characteristics start to revert to those found at lower TPP concentrations. This is due to the onset of efficient hole transport between the dopant molecules that reestablishes a transport imbalance. © 2001 American Institute of Physics.
UR - http://aip.scitation.org/doi/10.1063/1.1421415
UR - http://www.scopus.com/inward/record.url?scp=0035803363&partnerID=8YFLogxK
U2 - 10.1063/1.1421415
DO - 10.1063/1.1421415
M3 - Article
SN - 0003-6951
VL - 79
JO - Applied Physics Letters
JF - Applied Physics Letters
IS - 23
ER -