2017
DOI: 10.1080/08927022.2017.1296958
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Computationally connecting organic photovoltaic performance to atomistic arrangements and bulk morphology

Abstract: Rationally designing roll-to-roll printed organic photovoltaics requires a fundamental understanding of active layer morphologies optimized for charge separation and transport, and which ingredients can be used to self-assemble those morphologies. In this review article we discuss advances in three areas of computational modeling that provide insight into active layer morphology and the charge transport properties that result. We explain the computational bottlenecks prohibiting atomistically-detailed simulati… Show more

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Cited by 26 publications
(58 citation statements)
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References 149 publications
(179 reference statements)
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“…To characterize the molecular packings obtained in our simulations we use two structural metrics: an order parameter and simulated grazing incident X-ray scattering (GIXS) using the Diffractometer simulation software [35,69]. GIXS patterns are used to identify and quantify periodic morphological features and are used to validate predicted structures directly against experiments.…”
Section: Morphology Characterizationmentioning
confidence: 99%
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“…To characterize the molecular packings obtained in our simulations we use two structural metrics: an order parameter and simulated grazing incident X-ray scattering (GIXS) using the Diffractometer simulation software [35,69]. GIXS patterns are used to identify and quantify periodic morphological features and are used to validate predicted structures directly against experiments.…”
Section: Morphology Characterizationmentioning
confidence: 99%
“…At the largest scales, the structural evolution of 5 million coarsely-modeled P3HT monomers can be accessed on > 100 nm length-scales [34], but the computational cost of evaluating each step meant that equilibration was inaccessible over the 400 ns simulation trajectory. At 11-nm scales, equilibration of coarse-grained P3HT models are achievable over ∼2 µs simulation trajectories [28], but such coarse models miss the π-stacking details of P3HT rings, which can have implications for charge transport calculations [35,36]. Long relaxation times can be avoided in MD simulations through carefully selected initial conditions [32,[37][38][39][40], but these simulations can only check if a structure is locally stable, not whether it will robustly self-assemble at a particular state-point.…”
Section: Introductionmentioning
confidence: 99%
“…46 where the scattered intensity I at wave vector ⃗ q is related to the structure factor and the form factor P (⃗ q) as:…”
Section: Characterising Structure From Molecuar Dynamics (Md) Simulatmentioning
confidence: 99%
“…In [40]: from cme_utils.job_control import signac_helpers as diff diff_keys = diff.diff_jobs(data_path,'9e8bffd84a3fa9c262969f00552f4d08','4f8c0106906f219 e44fa45cd734a989c') In [46]: …”
Section: (Df['t']>200)and #Because Except One Of the Tajectories Out Ofmentioning
confidence: 99%
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