TY - JOUR
T1 - Dark carriers, trapping, and activation control of carrier recombination in Neat P3HT and P3HT
T2 - PCBM blends
AU - Ferguson, Andrew J.
AU - Kopidakis, Nikos
AU - Shaheen, Sean E.
AU - Rumbles, Garry
PY - 2011/11/24
Y1 - 2011/11/24
N2 - Using flash photolysis, time-resolved microwave conductivity we report the sub-200 ns photoconductivity transients for neat poly(3-hexylthiophene), P3HT, and four associated blends containing 1%, 5%, 20%, and 50%, by weight, of the soluble fullerene, [6,6]-phenyl-c61-butyric acid methyl ester, PCBM. We propose a detailed kinetic scheme that when solved numerically is consistent with all the data recorded as a function of excitation density and that describes the fate of mobile and trapped carriers in the system. In the neat polymer, mobile holes are the only contributor to the photoconductance transients, which decay according to first-order kinetics at all light intensities due to the presence of a large concentration of dark carriers present in the polymer. The signal decays with a characteristic rate constant (∼1 × 107 s-1) that describes the re-equilibration of trapped and mobile holes. In all four blends, the microwave absorption contains a significant contribution due to electrons in the PCBM clusters, even at the lowest blend ratio of 1%. The magnitude of the second-order rate coefficient, γb, for carrier recombination in all four blends (3.25 × 10-12 cm3 s-1 < γb < 10 × 10-12 cm3 s -1), and also that identified for the neat polymer, corresponds to a slow process that is not limited by diffusion but is activation controlled.
AB - Using flash photolysis, time-resolved microwave conductivity we report the sub-200 ns photoconductivity transients for neat poly(3-hexylthiophene), P3HT, and four associated blends containing 1%, 5%, 20%, and 50%, by weight, of the soluble fullerene, [6,6]-phenyl-c61-butyric acid methyl ester, PCBM. We propose a detailed kinetic scheme that when solved numerically is consistent with all the data recorded as a function of excitation density and that describes the fate of mobile and trapped carriers in the system. In the neat polymer, mobile holes are the only contributor to the photoconductance transients, which decay according to first-order kinetics at all light intensities due to the presence of a large concentration of dark carriers present in the polymer. The signal decays with a characteristic rate constant (∼1 × 107 s-1) that describes the re-equilibration of trapped and mobile holes. In all four blends, the microwave absorption contains a significant contribution due to electrons in the PCBM clusters, even at the lowest blend ratio of 1%. The magnitude of the second-order rate coefficient, γb, for carrier recombination in all four blends (3.25 × 10-12 cm3 s-1 < γb < 10 × 10-12 cm3 s -1), and also that identified for the neat polymer, corresponds to a slow process that is not limited by diffusion but is activation controlled.
UR - http://www.scopus.com/inward/record.url?scp=81755177599&partnerID=8YFLogxK
U2 - 10.1021/jp208014v
DO - 10.1021/jp208014v
M3 - Article
AN - SCOPUS:81755177599
VL - 115
SP - 23134
EP - 23148
JO - Journal of Physical Chemistry C
JF - Journal of Physical Chemistry C
SN - 1932-7447
IS - 46
ER -