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Subnanosecond Charge Recombination Dynamics in P3HT/PC(61)BM Films

Ultrafast near-infrared absorption spectroscopy was used to investigate the influence of film morphology and excitation photon energy on the charge recombination (CR) dynamics in the initial nanosecond timescale in the P3HT/PC(61)BM blend films. With reference to the CS(2)-cast films, the solvent va...

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Detalles Bibliográficos
Autores principales: Zhang, Wei, Zhao, Ning-Jiu, Huo, Ming-Ming, Fu, Li-Min, Ai, Xi-Cheng, Zhang, Jian-Ping
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2012
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6268940/
https://www.ncbi.nlm.nih.gov/pubmed/23178308
http://dx.doi.org/10.3390/molecules171213923
Descripción
Sumario:Ultrafast near-infrared absorption spectroscopy was used to investigate the influence of film morphology and excitation photon energy on the charge recombination (CR) dynamics in the initial nanosecond timescale in the P3HT/PC(61)BM blend films. With reference to the CS(2)-cast films, the solvent vapor annealed (SVA) ones show 2–3-fold improvement in hole mobility and more than 5-fold reduction in the polymer-localized trap states of holes. At Δt = 70 ps, the hole mobility (μ(h)) and the bimolecular CR rate (γ(bi)) of the SVA films are μ(h) = 8.7 × 10(−4) cm(2)·s(−1)·V(−1) and γ(bi) = 4.5 × 10(−10) cm(3)·s(−1), whereas at Δt = 1 ns they drop to 8.7 × 10(−5) cm(2)·s(−1)·V(−1) and 4.6 × 10(−11) cm(3)·s(−1), respectively. In addition, upon increasing the hole concentration, the hole mobility increases substantially faster under the above-gap photoexcitation than it does under the band-gap photoexcitation, irrespective of the film morphologies. The results point to the importance of utilizing the photogenerated free charges in the early timescales.