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ORGANICPV

light is absorbed in an organic semiconductor, the energy produces a neutral quasiparticle, or exciton, rather than free charge carriers. In most organic solar cells, the exciton is typically dissociated into free charges at the interface between two different organic semiconductors with different electron affinities, hence the widespread use of donor/acceptor blends.

However, while the active layer of an organic solar cell needs to be ~100-200 nm thick to absorb most of the incident light, the diffusion length of an exciton is ~10 nm,7, 8

and thus the donor and

acceptor materials must be mixed on this length scale to yield an efficient device.

Analysis of this nanoscale morphology requires high-resolution spatial mapping of the active layer, particularly using scanning probe techniques such as atomic force microscopy (AFM) and its various extensions. Scanning probe microscopy is especially useful because of the ability to image at

50

resolutions approaching the ~10-100 nm scale of the domains observed in common OPV materials. Several groups have, for example, analyzed OPV systems using AFM,9, 10

electrostatic force microscopy (EFM),11

conducting AFM,11, 12 and

scanning Kelvin probe microscopy (SKPM).13-16 Optical variations such as near-field scanning optical microscopy (NSOM)17, 18 luminescence-based AFM19 probe OPV blend morphology.

and tunneling have also been used to

We have recently reviewed the broad use of scanning probe microscopy in the field of organic electronics20

and identified specific areas of

nanoscale physics that are important to OPV operation.21

In this article, we take a more practical turn and discuss the experimental challenges and opportunities associated with two different AFM techniques, photoconductive AFM (pcAFM)22, 23 time-resolved EFM (trEFM),24

that have been used

help understand how morphology impacts OPV performance.

Figure 1. (A)

Schematic of a typical bulk heterojunction organic photovoltaic device. Schematic diagrams of the (B) trEFM and (C) pcAFM experimental setups based on Asylum Research’s MFP 3D- AFM system

trEFM is a non-contact technique that utilizes time- resolved measurements on OPV layers to analyze the local variations in photoinduced charge generation, collection, and discharge, while pcAFM is a contact-mode method that measures the photocurrent directly to obtain useful information of the local morphology and its relation to the local photoresponse. Figure 1b and 1c show a schematic diagram of the instrumentation used in trEFM and pcAFM. In our lab, we have implemented both techniques using Asylum Research’s MFP-3D-BIO AFM coupled to a Nikon TE2000-U inverted optical microscope and controlled using a custom code suite written in Igor (WaveMetrics, Inc.), the scientific software environment used by Asylum Research’s AFMs . The system is mounted on an optical breadboard to accommodate external optics (Thor Labs) and is supported by a passive vibration isolation stage (Minus K Technology). Neutral density (ND) filters allow us to adjust the illumination intensity in both techniques. The entire system is housed within a plywood box with copper mesh shielding and acoustic-damping foam. In order to protect potentially air-sensitive samples from photo- oxidation, we use an Asylum Research sealed fluid cell. Originally designed for imaging biological samples under liquid, the design permits the loading of sensitive samples into the cell in a glovebox and allows us to perform measurements while purged with dry nitrogen. This approach obviates the need to install the entire AFM/optical system in a glovebox.

and

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