OPTOELECTRONIC DEVICES, LOW TEMPERATURE PREPARATION METHODS, AND IMPROVED ELECTRON TRANSPORT LAYERS

Abstract

An optoelectronic device such as a photovoltaic device which has at least one layer, such as an electron transport layer, which comprises a plurality of alternating, oppositely charged layers including metal oxide layers. The metal oxide can be zinc oxide. The plurality of layers can be prepared by layer-by-layer processing in which alternating layers are built up step-by-step due to electrostatic attraction. The efficiency of the device can be increased by this processing method compared to a comparable method like sputtering. The number of layers can be controlled to improve device efficiency. Aqueous solutions can be used which is environmentally friendly. Annealing can be avoided. A quantum dot layer can be used next to the metal oxide layer to form a quantum dot heterojunction solar device.

Claims

1. A photovoltaic device comprising: at least two electrodes including at least one anode and at least one cathode, and at least one electron transport layer between the two electrodes, wherein the electron transport layer comprises alternating, oppositely charged layers.

2. The photovoltaic device of claim 1, wherein the device is an organic photovoltaic device.

3. The photovoltaic device of claims 1-2, wherein the electron transport layer comprises a plurality of bilayers.

4. The photovoltaic device of claims 1-3, wherein the electron transport layer comprises metal oxide.

5. The photovoltaic device of claims 1-4, wherein the electron transport layer comprises metal oxide and the metal oxide is a nanoparticulate metal oxide.

6. The photovoltaic device of claims 1-5, wherein the electron transport layer further comprise at least one polyelectrolyte.

7. The photovoltaic device of claims 1-6, wherein the electron transport layer comprises at least one positively charged metal oxide layer and at least one negatively charged polyelectrolyte layer.

8. The photovoltaic device of claims 1-7, wherein the electron transport layer includes 2-6 bilayers.

9. The photovoltaic device of claims 1-8, wherein the electron transport layer is not annealed.

10. The photovoltaic device of claims 1-9, wherein the photovoltaic device has an inverted structure.

11. A method comprising: fabricating at least one photovoltaic device according to claims 1-10, wherein the electron transport layer is prepared by layer-by-layer deposition.

12. The method of claim 11, wherein the electron transport layer is not annealed.

13. The method of claims 11-12, wherein the number of layers in the electron transport layer is selected to maximize device efficiency.

14. The method of claims 11-13, wherein the layer-by-layer deposition is carried out with use of inks.

15. The method of claim 11-14, wherein the electron transport layer is prepared by deposition of aqueous solutions and drying.

Description

BRIEF DESCRIPTION OF THE FIGURES

[0034] FIGS. 1A-B illustrate for one embodiment (A) an architecture of an inverted bulk heterojunction solar device (B) employing ZnO layer assembled at room temperature using the LbL technique. More particularly, FIGS. 1A and 1B illustrate (A) the device architecture of a layer-by-layer ZnO NP/poly(benzo[1,2-b:4,5-b′]dithiophene-thieno[3,4-c]pyrrole-4,6-dione) (PBDTTPD)/[6,6]-phenyl C.sub.61 butyric acid methyl ester (PCBM) ordered bulk hetero-junction solar cell. (B) the layer-by-layer structure consisting of multilayers of polyacrylic acid (PAA) and ZnO nanoparticles.

[0035] FIG. 2 illustrates for one embodiment an AFM height image of the prepared ZnO film before (upper) and after (lower) coating with the polymer hetero-junction.

[0036] FIG. 3 illustrates for one embodiment the effect of annealing and ZnO film thickness (number of bilayers) on the resulting device efficiency.

[0037] FIG. 4 illustrates for one embodiment film thickness and surface roughness as a function of number of bilayers.

[0038] FIG. 5 illustrates for one embodiment the power conversion efficiency as a function of film thickness for the LbL films (layer by layer) compared to sputtered films.

[0039] FIG. 6 illustrates for one embodiment the layer by layer technique to form a ZnO film onto ITO glass, a layer of PbS—as a donor—was coated on the surface of ZnO which works as acceptor.

[0040] FIG. 7 illustrates for one embodiment time resolved laser spectroscopy used to investigate the electron transfer at the PbS—ZnO interface.

[0041] FIGS. 8a-c illustrate (a) Changes in the thickness and root mean square (RMS) roughness of the surface with increasing number of bilayers, (b) and (c) AFM height images of one bilayer and five bilayers of ZnO/PAA thin films, respectively, on silica substrates.

[0042] FIGS. 9a-b illustrate (a) the UV-Vis absorption spectrum of a polymer BHJ on top of a five-bilayer ZnO/PAA thin film. (b) The corresponding AFM height image of the same device showing the active polymer layer covering the surface of the ZnO nanoparticles and filling the pores in between.

[0043] FIGS. 10a-d illustrate inverted BHJ solar cells fabricated from the PBDTTPD derivatives, under AM1.5G illumination; cast from CB, with 5% (v/v) CN additive showing (a) solar cell PCEs of the as-prepared and annealed ETLs as a function of the number of layers, (b) PCE as a function of ETL thickness, (c) characteristic J-V curves and (d) external quantum efficiency (EQE) spectra of sputtered and LbL ZnO/PAA ETL-containing devices.

[0044] FIGS. 11a-b illustrate (a) C1s XPS spectra of a four-bilayer ZnO/PAA as-prepared and annealed thin film at 300° C. in air for one hour; (b) ATR-FTIR spectra of the as-prepared and annealed ZnO/PAA films showing the band of the free carboxylate group.

DETAILED DESCRIPTION

Introduction

[0045] All references cited herein are incorporated by reference in their entireties.

[0046] U.S. priority provisional application 62/108,430 filed Jan. 27, 2015 is incorporated herein by reference in its entirety.

[0047] The reference, Eita et. A I, Small, 2015, 11, 1, 112-118, is hereby incorporated by reference in its entirety for all purposes, including working examples and figures.

[0048] The reference, Eita et. A I., Adv. Fund. Mat., 2015, 25, 10, 1558-1564, is hereby incorporated by reference in its entirety for all purposes, including working examples and figures.

Devices

[0049] A wide variety of optoelectronic devices are known in the art. They can convert light into electricity, for example, or they can convert electricity into light, wherein the term light is used expansively to mean a broader range of the electromagnetic spectrum than mere visible light. The light can be, for example, visible, infrared, or ultraviolet. For example, photovoltaic devices are described in, for example, Organic Photovoltaics, Mechanisms, Materials, and Devices, (Sun and Sariciftci, Eds.), CRC, 2005. In addition, light emitting devices are described in, for example, Organic Light-Emitting Materials and Devices, (Li, Meng, Eds.), CRC, 2007. Organic types of devices can be made, wherein one or more layers including the active layer includes an organic component. In many cases, the devices will comprise one or more semiconducting materials or semiconducting layers.

[0050] In addition to classical photovoltaic devices, other kinds of photovoltaic devices are known in the art such as, for example, photodetectors and light-harvesting devices. Other types of optoelectronic and/or photovoltaic devices include, for example, semiconducting lasers, LEDs, photodiodes, phototransistors, photomultipliers, optoisolators, integrated optical circuit (IOC) elements, photoresistors, photoconductive camera tubes, and charge-coupled imaging devices.

[0051] Photovoltaic devices and solar cells, which are preferred embodiments, are known in the art. See, for example: (1) Cho et al., Sci. Rep., 4, doi: 10.1038/srep04306, 2014; (2) Tan et al., ACS Applied Materials & Interfaces 5, 4696-4701, doi: 10.1021/am303004r (2013); (3) Park et al., J. Mater. Chem., A1 6327-6334, doi: 10.1039/C3TA10637C (2013); (4) Sung et al., Sol. Energy Mater. Sol. Cells, 98, 103-109, doi: http://dx.doiorg/10.1016/j.solmat.2011.10.021 (2012); (5) Hau et al., Appl. Phys. Lett., 92, -, doi: doi: http://dx.doi.org/10.1063/1.2945281 (2008); and (6) Peiro et al., J. Mater. Chem. 16, 2088-2096 (2006).

[0052] See also, for example: (1) Repins, I. et al. 19.9%-efficient ZnO/CdS/CuInGaSe2 solar cell with 81.2% fill factor. Progress in Photovoltaics: Research and Applications 16, 235-239, doi:10.1002/pip.822 (2008); (2) Bouclé, J., et al., Simple Approach to Hybrid Polymer/Porous Metal Oxide Solar Cells from Solution-Processed ZnO Nanocrystals. The Journal of Physical Chemistry C 114, 3664-3674, doi:10.1021/jp909376f (2010); (3) Anta, J. A., et al., ZnO-Based Dye-Sensitized Solar Cells. The Journal of Physical Chemistry C 116, 11413-11425, doi:10.1021/jp3010025 (2012); (4) Beek, W. J. E., et al., Efficient Hybrid Solar Cells from Zinc Oxide Nanoparticles and a Conjugated Polymer. Advanced Materials 16, 1009-1013, doi:10.1002/adma.200306659 (2004); (5) Law, M., et al., Nanowire dye-sensitized solar cells. Nat Mater 4, 455-459, doi:http://www.nature.com/nmat/journal/v4/n6/suppinfo/nmat1387_S1.html (2005); (6) Jean, J. et al. ZnO Nanowire Arrays for Enhanced Photocurrent in PbS Quantum Dot Solar Cells. Advanced Materials 25, 2790-2796, doi:10.100.sup.2/adma.201204192 (2013); (7) Wang, H., et al., PbS-Quantum-Dot-Based Heterojunction Solar Cells Utilizing ZnO Nanowires for High External Quantum Efficiency in the Near-Infrared Region. The Journal of Physical Chemistry Letters 4, 2455-2460, doi:10.1021/jz4012299 (2013); (8) Liu, D. & Kelly, T. L. Perovskite solar cells with a planar heterojunction structure prepared using room-temperature solution processing techniques. Nat Photon advance online publication, doi:10.1038/nphoton.2013.342. http://www.nature.com/nphoton/journal/vaop/ncurrent/abs/nphoton.2013.342.html#supplementary-information (2013).

[0053] A wide variety of photovoltaic devices can be used as described herein including, for example, organic photovoltaic devices, dye-sensitized photovoltaic devices, quantum dot photovoltaic devices, hybrid photovoltaic devices, and photovoltaic devices including a bulk heterojunction (BHJ) in the active layer. For example, the active layer can comprise at least donor material, such as a conjugated polymer, and at least one acceptor material such as a fullerene derivative such as, for example, PCBM. The PCBM can be a C60 PCBM (PC.sub.60BM or PC.sub.61BM) or a C70 PCBM (PC.sub.70BM or PC.sub.71BM) as known in the art. The conjugated polymer can be, for example, a donor-acceptor polymer. The polymers can be soluble and can be derivatized to encourage solubility. Inverted photovoltaic devices can be made and used. Photovoltaic devices can be powered by natural light or artificial light.

[0054] For polymer photovoltaic devices, Yip et al., Energy Environ. Sci., DOI: 10.1039/c2ee02806a, describes solution processing of interfacial materials including descriptions for use of metal oxides such as ZnO and TiO.sub.2.

[0055] The devices, as is known in the art, can comprise at least two electrodes including at least one cathode and at least one anode. An active layer can be between the electrodes in which the active layer is where charges, whether holes or electrons or combinations of holes and electrons, are created for current flow. One or more of interfacial layers can be used between the electrode and the active layer to facilitate charge transport and/or charge injection. Interfacial layers can also block a particular type of charge flow. Examples include electron transport layers (ETLs) and hole transport layers (HTLs).

[0056] Device substrates can be used as known in the art including rigid and flexible substrates such as glass or polymer substrates, respectively. Substrates can be cleaned and dried. Substrates can be coated with a positively or negatively charged layer, including a polymer layer, to facilitate further building up of charged layers. For example, a substrate can be coated with a positively charged polymer such as poly(allylamine hydrochloride).

[0057] Transparent conductive oxides such as ITO can be used as known in the art to provide a transparent conductive electrode.

[0058] Transparent photovoltaic devices can be made and used, for example, in building windows. Transparent donor can be used with transparent acceptor.

[0059] The use of antireflective layers can be avoided in some embodiments described herein.

Electron Transporting Layer

[0060] In optoelectronic devices, electron transporting layers (ETLs) are known in the art. See, for example, US Patent Publications 2011/0308613 to Tseng et al; 2014/0137929 to Yun et al.; and 2013/0019937 to So et al.; See also, for example, WO 2012/168700; WO 2013/167224. The ETL can also have a hole blocking function.

[0061] The electron transporting layer can itself comprise one or more, two or more sub-layers including bi-layers.

[0062] The thickness of the ETL can be, for example, about 1 to about 250 nm, or about 5 nm to about 100 nm, or about 10 nm to about 50 nm.

[0063] ETL materials and fabrication methods are described further herein.

Layer-by-Layer Deposition

[0064] Layer-by-layer (LbL) deposition is known in the art. See, for example, Eita et al., J. Phys. Chem. C, 2012, 116, 4621-4627; and Benten et al., Thin Solid Films, 517 (2009) 2016-2022. See also, Multilayer Thin Films: Sequential Assembly of Nanocomposite Materials, (Decher, Schlenoff, Eds.), Wiley-VCH: 2003. In this process, alternating, oppositely charged layers are deposited. A positive layer can be deposited, followed by deposition of a negatively charged layer, and this process can be repeated to build up bi-layers. The thickness of the layer can be controlled by controlling the number of bilayers.

[0065] The number of bi-layers can be selected so as to optimize a property such as device efficiency. For example, the number of bi-layers can be 2-6, or 3-5.

[0066] Layers can be rinsed in a liquid such as water before deposition of the next layer.

[0067] Dipping processes can be used including processes controlled by robots, software, and automation.

[0068] The layers can be porous which encourages good interfacial contact and high surface area which can facilitate good charge transfer.

Metal Oxides

[0069] Metal oxides are known in the art and can be semiconductors, and semiconductive layers can be prepared. The metal of the oxide can be a wide variety of metals including transition metals as long as they provide the needed function in, for example, an ETL. Metal oxides are used such as titanium dioxide or zinc oxide as these materials provide for high transparency over a broad frequency range and good electron mobility. Materials which provide good electron mobility are preferred.

[0070] The metal oxide can be in the form of a nanoparticle, or in other words, nanoparticulate metal oxides can be used. For a nanoparticle, the metal oxide can be used in conjunction with a surfactant to stabilize the solid in dispersed form in a solution. The surfactant can be a cationic or anionic surfactant. An example is a functionalized silane compound such as, for example, 3-aminopropyl triethoxysilane. The average particle size can be, for example, about 1 to about 100 nm, or about 1 nm to about 50 nm.

Polyelectrolytes

[0071] Polyelectrolytes are known in the art, and they can be positively or negatively charged with the counterion to balance the charge of the polymer. The polyelectrolyte can comprise an uncharged backbone with charged side groups. For example, one can have an all carbon backbone with side groups comprising a negatively charged side group such as, for example, a carboxylic moiety, such as poly(acrylic acid) (PM). The counterion of the polyelectrolyte is not particularly limited but can be, for example, an alkali metal such as sodium or potassium.

[0072] Another example of a polyelectrolyte is poly(allylamine hydrochloride) (PAH) which is a positively charged polyelectrolyte. PAH is positively charged and can be used, for example, as a precursor layer directly placed on ITO to achieve enough positive charge for the adsorption of the negatively charge PAA. Without PAH, PAA adsorption is weak and the whole film thickness and hence device efficiency can be dramatically reduced.

[0073] The number average molecular weight of the polyelectrolyte can be, for example, 1,000 to 100,000 g/mol, or 5,000 to 50,000 g/mol, or 10,000 to 25,000 g/mol.

Nanocomposite

[0074] The combination of metal oxide, in nanoscale or nanoparticulate form, and polyelectrolyte can provide for a nanocomposite. See, Multilayer Thin Films: Sequential Assembly of Nanocomposite Materials, (Decher, Schlenoff, Eds.), Wiley-VCH: 2003.

Solvent Carrier

[0075] The metal oxide can be in particulate form, including nanoparticulate form, and can be dispersed in a solvent carrier or a liquid carrier. This can provide an ink. The solvent carrier is used to disperse the solid particles and can comprise one or more solvents including water and solvents miscible with water. The solvent carrier can be an aqueous based solvent carrier in which either water is the only solvent used or water is by weight percent the majority solvent present, even if mixed with one or more solvents mixed with the water.

[0076] The pH of the aqueous solution or dispersion can be controlled as needed, and can be below 7 or above 7. For example, pH can be 6 to 9. The pH of the metal oxide solution or dispersion can be less than 7 (e.g., 6-7) and the pH of polyelectrolyte solution or dispersion can be more than 7 (e.g., 7-9).

[0077] One or more salts, such as NaCl, can be added to the aqueous solution. For example, a 0.1 M NaCl solution can be added to, for example, the polyelectrolyte solution.

Quantum Dot Layer

[0078] In some embodiments, the device can also comprise an additional layer in contact with the layer prepared by the LBL method such as the electron transport layer. For example, the device can also comprise at least one quantum dot layer in contact with the layer. For example, PbS quantum dots can be used in such a layer. The materials can also be called a semiconductor nanocrystal. See, for example, US Patent Publication 2010/0265307.

[0079] The quantum dots can provide for absorption and harvesting of light all over the solar spectrum range from the visible to infrared regions.

[0080] If useful, use of the quantum dot layer can mean that highly efficient electron transfer can be measured.

Method of Fabricating the Devices

[0081] The devices described herein can be prepared by methods including a method comprising: fabricating at least one optoelectronic device according to one or more embodiments described herein, wherein the layer is prepared by layer-by-layer deposition. In particular, the optoelectronic device can be a photovoltaic device, and the layer can be an ETL in the photovoltaic device.

[0082] The layers can be subjected to post-deposition processing such as annealing including thermal annealing. The layer can be annealed or can be not annealed, although often it is desired if possible to avoid annealing and other post-deposition treatments. If the layer is not annealed, device properties such as device efficiency can be increased. If the layer is annealed, the annealing temperature in thermal annealing can be, for example, 150° C. to 350° C.

[0083] The number of layers or bilayers can be selected to maximize device efficiency.

[0084] In one embodiment, the layer is prepared by deposition of aqueous solutions or dispersions (alternatively called inks) and drying. For example, an aqueous solution of polyelectrolyte can be used, and an aqueous solution of metal oxide can be used.

[0085] The ink composition can “comprise,” or can “consist essentially of,” or can “consist of” the materials, compounds, and/or polymers to provide the desired device with the novel features.

Device Properties

[0086] The device properties can be measured by methods known in the art. For example, for a photovoltaic device, the power conversion efficiency (PCE) can be measured along with fill factor (FF), open circuit voltage (V.sub.oc), and short circuit current density (J.sub.sc). The power conversion efficiency can be, for example, at least 4% or at least 5% or at least 6%. The fill factor can be, for example, at least 45%, or at least 50%, or at least 55%. The J.sub.sc value can be, for example, at least 10, or at least 11, or at least 12 mA/cm.sup.2. As known in the art, a series of devices can be measured and the results averaged, while also a maximum measurement is identified.

Other Applications

[0087] Other applications can be found for the inventive layers described herein, particularly those which benefit from high porosity and high interfacial contact, which include, for example, catalysis and membranes.

WORKING EXAMPLES

[0088] Additional embodiments are provided in the following non-limiting working examples.

Example 1

[0089] A new polymer-ZnO solar cell device was prepared. The device was based on room-temperature solution-processed methods to prepare the ZnO thin film which acts as an ETL in the device. Preparing ZnO thin film using the new method has introduced an enhancement of the device efficiently yielding, for example, 6% which is favorable to the same device components using ZnO prepared by the sputtering technique. Moreover, the ZnO thin film is prepared at room temperature, which often is a basic requirement in flexible solar cell fabrication.

[0090] Comparative devices prepared by sputtering, rather than LbL, were prepared by standard methods including radiofrequency sputtering in high vacuum using argon plasma and ZnO targets without any temperature change.

[0091] The following Table 1 provides final values for both LbL samples and sputtered samples after light soaking (in “light soaking,” one leaves the ZnO layer in white light overnight before coating the active polymer layer):

TABLE-US-00001 TABLE 1 J.sub.SC V.sub.OC FF Avg. PCE Max. PCE [mA/cm.sup.2] [V] [%] [%] [%] Number of bilayers LbL 4 bilayers 12.4 0.87 55 5.6 6.0 ZnO sputtered thickness [nm]  5 12.3 0.80 49 4.1 4.8 10 12.2 0.85 49 4.6 5.1 15 12.0 0.81 45 4.0 4.6 30 11.8 0.83 50 4.2 4.9

[0092] FIG. 1 shows the architecture and components of the solar device. FIG. 1(A) shows an inverted bulk heterojunction solar device employing ZnO layer assembled at room temperature. The layer-by-layer structure of the ZnO layer is shown in FIG. 1(B).

[0093] After assembly of ZnO nanoparticles on the surface, a mixture of donor (PBDTTPD) and acceptor (PC.sub.71BM) was spin-coated on the surface to form a bulk hetero-junction device. FIG. 2 shows the AFM height image of the prepared ZnO thin film before and after coating with the polymer hetero-junction. FIG. 2 confirms the coating of the active polymer layer on the surface of ZnO nanoparticles and diffusing into its porous structure, as a sign of good and increased interfacial contact.

[0094] The effect of annealing and ZnO film thickness on the resulting device efficiency was investigated, Table 2 and FIG. 3. The not-annealed ZnO films gave higher efficiency—about double—than the ones annealed at 300° C. for one hour in air. ZnO bilayers were coated with different bilayers number from 1 to 5. The device efficiency increases with increasing the film thickness (number of bilayers) until it reaches a plateau at 3 and 4 bilayers for the annealed and not annealed films, respectively. The 3 and 4 bilayers film thickness are 22 nm and 25 nm, respectively, as measured by ellipsometry. The device gives a maximum efficiency of 6% with a fill-factor (FF) of 55%, and comparably high short-circuits currents (J.sub.sc) of more than 12 mA/cm.sup.2.

TABLE-US-00002 TABLE 2 Number Polymer of ID Structure Bilayers PCE % FF V.sub.oc J.sub.SC EA6 PBDTTPD 1 4 44 0.82 11.2 (EH/C8) EA6 PBDTTPD 1.5 4.14 48 0.75 11.5 (EH/C8) EA6 PBDTTPD 2 4 44 0.76 11.7 (EH/C8) EA6 PBDTTPD 2.5 4.6 50 0.83 11.2 (EH/C8) EA6 PBDTTPD 3 4.84 51 0.85 11.1 (EH/C8) EA6 PBDTTPD 3.5 5.17 53 0.86 11.4 (EH/C8) EA6 PBDTTPD 4 5.33 55 0.87 11.1 (EH/C8) EA6 PBDTTPD 4.5 5.07 55 0.85 10.9 (EH/C8) EA6 PBDTTPD 5 4.94 54 0.87 10.4 (EH/C8) EA6 PBDTTPD 5.5 4.9 53 0.85 10.9 (EH/C8) EA6 PBDTTPD 6 4.68 52 0.84 10.8 (EH/C8) EA6 PBDTTPD 1 2.6 38 0.6 11.5 Annealed (EH/C8) EA6 PBDTTPD 2 2.58 39 0.56 11.9 Annealed (EH/C8) EA6 PBDTTPD 3 3.47 45 0.63 12 Annealed (EH/C8) EA6 PBDTTPD 4 3.5 45 0.66 11.6 Annealed (EH/C8) EA6 PBDTTPD 5 3.23 45 0.65 11.1 Annealed (EH/C8) EA6 PBDTTPD 6 3.7 48 0.7 10.9 Annealed (EH/C8)

[0095] Structures of the active layer are shown below. EH/C8 is ethylhexyl substitutent on the polymer PBDTTPD (Poly(benzo[1,2-b:4,5-b′]dithiophene-alt-thieno[3,4-c]pyrrole-4,6-dione (PBDTTPD).

##STR00001##

[0096] FIGS. 4 and 5 provide additional data for the novel devices. FIG. 4 demonstrates how thickness and surface roughness increased with the number of layers. FIG. 5 shows how higher efficiency can be found with use of the LbL method compared to sputtering.

Example 2

[0097] In another example, the zinc oxide layer-by-layer (LbL) approach was used in conjunction with a lead sulfide (PbS) layer. See FIGS. 6 and 7. See also Eita et. A I., Small, 2015, 11, 1, 112-118 for additional description.

[0098] The ZnO used here was dispersed in cationic surfactant; the PAA is of low molecular weight 15,000 g/mol; the pH of the solutions is kept at the native value at 6.7 and 8.3 for ZnO and PAA, respectively. A 0.1 M NaCl was added to the PAA solution. Cleaning the ITO substrates was done by successive sonication in 0.1 M NaOH, 2-propanol and finally acetone, and then substrates were dried with N.sub.2 gas. Substrates were immersed in a solution of poly-allylamine hydrochloride (PAH) to coat a positively charged layer on the ITO glass first. A standard LbL method was applied; substrates were immersed in PAA and ZnO for 10 minutes each, having three rinsing steps in ultrapure water for 2 minutes each. Different thicknesses were obtained depending on the number of layers.

[0099] Lead sulfide (PbS) quantum dots (QDs) is a known donor in solar cells research. Hence, PbS was coated on top of ZnO in order to investigate the efficiency of the ZnO film to accommodate PbS and to act as an acceptor in solar cells. See FIG. 6. Coating of PbS QDs was achieved by dipping the ZnO-coated substrates in the PbS QDs dispersion in hexane, withdrawing and letting to dry in the fume hood for seconds, then dipping in ethandithiol (EDT)—as a cross-linker to bind the QDs with each other to produce a uniform film—withdrawn, and letting to dry for seconds.

[0100] The ZnO—PbS films were characterized by ellipsometry, atomic force microscopy (AFM) and scanning electron microscopy (SEM) to get a full picture about the film thickness, morphology, roughness and the interfacial contact. It was found that the films have porous structure that is growing with increasing the film thickness. Due to the porous structure, the interfacial contact between ZnO and PbS is maximized so that PbS QDs are adsorbed everywhere onto the ZnO. The electron transfer dynamics, and hence the efficiency of the film to act as an acceptor layer, was investigated by ultrafast time-resolved laser spectroscopy. See FIG. 7.

[0101] Electron transfer from the highest energy levels of PbS to the conduction band of ZnO without relaxation was monitored by means of transient absorption spectroscopy. This effect means that the PbS as electron absorber could harvest light all over the visible or the solar spectrum and transfer all these excited electrons to ZnO at the same time giving rise to an estimated higher solar cell efficiency. The electron transfer is supported by the higher interfacial contact between PbS and ZnO.

Supplemental Description and Embodiments

[0102] As described above, and as further described below, the use of metal oxide interlayers in polymer solar cells has many advantages because metal oxides are abundant, thermally stable, and can be used in flexible devices. Here, a layer-by-layer (LbL) protocol is described as a facile, room-temperature, solution-processed method to prepare electron transport layers from commercial ZnO nanoparticles and polyacrylic acid (PAA) with a controlled and tunable porous structure, which provides large interfacial contacts with the active layer. Applying this LbL approach to bulk heterojunction polymer solar cells with an improved ZnO layer thickness of ca. 25 nm yields solar cell power-conversion efficiencies (PCEs) of ca. 6%, exceeding the efficiency of amorphous ZnO interlayers formed by conventional sputtering methods. Interestingly, annealing the ZnO/PAA interlayers in nitrogen and air environments in the range of 100-300° C. reduces the device PCEs by almost 20 to 50%, indicating the importance of conformational changes inherent to the PAA polymer in the LbL-deposited films to solar cell performance. This protocol suggests a new fabrication method for solution-processed polymer solar cell devices that does not require post-processing thermal annealing treatments and that is applicable to flexible devices printed on plastic substrates.

[0103] An alternative technique that can be used to control the interfacial contacts is the room-temperature layer-by-layer (LbL) method. Using this method, as described above, the inventors created porous structures within the ZnO NP layers on which quantum dots, for example, could be incorporated as the light absorber layer..sup.[36]

[0104] Here, the assembly and performance of a ZnO NPs/poly(benzo[1,2-b:4,5-b′]dithiophene-thieno[3,4-c]pyrrole-4,6-dione) (PBDTTPD)/[6,6]-phenyl C.sub.61 butyric acid methyl ester (PCBM) BHJ solar cell is described with the device architecture shown in FIG. 1A. The inventors prepared the ZnO-based ETL by using a LbL approach based on a ZnO/polyacrylic acid (PAA) multilayered structure deposited from aqueous solutions (FIG. 1B). This approach allowed the ZnO/PAA thickness and the porous structure to be tuneable..sup.[36] The inventors examined the film build-up and surface morphology of the ZnO ETL by ellipsometry and atomic force microscopy (AFM). The inventors made the polymer-fullerene BHJ device by spin-coating an active layer of PBDTTPD and PCBM onto the LbL-deposited ZnO/PAA thin film. PBDTTPDs are among the best-performing polymer donors for BHJ solar cells with PCBM acceptors, yielding high V.sub.OC>0.9 V, high FFs of ca. 70%, and PCEs>6% in direct device configurations..sup.[37-43] The inventors used PBDTTPD-based BHJ solar cells as a model system to show that the performance of inverted BHJ devices with ZnO-based interlayers depends on the thickness of the ZnO layer deposited by the LbL approach. The inventors show that as-prepared LbL-deposited ZnO/PAA solar cells yield comparably high figures of merit: J.sub.SC as high as 12.4 mA cm.sup.−2, V.sub.oc of 0.87 V, FF of 55%, and PCE of 6.0% at an optimized ZnO layer thickness of 25 nm. Interestingly, the performance of our as-prepared BHJ solar cells at room temperature was better than that of thermally annealed devices, indicating the importance of conformational changes of the PAA polymer in the LbL-deposited films to solar cell performance.

[0105] Thin films of ZnO/PAA ETL under optimized conditions were prepared according to a previously described LbL method for implementation in polymer BHJ devices..sup.[36,44] FIG. 8a shows the film thickness as a function of the number of ZnO/PAA bilayers as measured by ellipsometry, demonstrating a progressive thickness variation starting at 13 nm for one bilayer and reaching 29 nm for five bilayers. AFM height images for one and five bilayer(s) are shown in FIGS. 8b and 8c, respectively. In the one-bilayer thin film, the ZnO NPs cover the substrate in a densely packed manner. In addition, the inventors also measured the film thickness by AFM step analysis for comparison, and found that the thicknesses of the 1 and 5 bilayer samples may be approximated to ca. 12 and 30 nm, respectively, which are comparable to those measured by ellipsometry.

[0106] The ZnO NPs are irregular in shapes with ˜20 nm in sizes as apparent in transmission electron microscopy (TEM) image. whereas the hydrodynamic radius is 99 nm as measured by dynamic light scattering (DLS) in solution..sup.[44] These results suggest that ZnO NPs are always associated with water and surfactant molecules, and hence several associated ZnO NPs co-adsorb together onto the surface as seen in the AFM image. By increasing the number of bilayers, the nanoparticles tend to assemble to form a nanoporous structure as seen in the AFM image in FIG. 8c. The surface roughness as measured by AFM increases as the number of bilayers increases as shown in FIG. 8a. Apparently, the surface roughness is high at a given film thickness, e.g., the five-bilayer film is 29 nm thick while its surface roughness is 14.2 nm. The overall thickness of the film is lower compared to the average particle size of ZnO NPs. This observation was reported previously and is due to imperfections in the multilayer structure..sup.[41] Adsorption happens at the beginning of the process in separate domains. The porous structure is hence formed from the beginning. By increasing the number of bilayers, the porous structure grows and thus the overall film thickness is low. Given that ZnO nanoparticles are granular and not spherical, the film build-up is not a consequence of the particle size in the Z-direction. There is a three-dimensional build-up of granules that could fit everywhere in the porous structure rather than growing only in the Z-direction giving rise to the low thickness reported by ellipsometry (FIG. 8a) and by AFM. On the other hand, in such colloidal domain, smaller charged particles reach the surface easier and faster than bigger particles. It is apparent then that the overall film thickness is not necessarily correlated with the ZnO particle size.

[0107] Thin-film BHJ solar cells with an inverted configuration of ITO/ZnO/PBDTTPD: PC.sub.71 BM/MoO.sub.3/Ag were fabricated with ZnO/PAA ETLs prepared by the LbL technique. Cells with optimized active layers of PBDTTPD:PC.sub.71BM in a blend ratio of 1:1.5 (wt/wt) were cast from chlorobenzene (CB) with 5% (v/v) of the processing additive 1-chloronaphthalene (CN).

[0108] FIG. 9a shows the UV-Vis absorption spectrum of the BHJ device. The spectrum shows the absorption peak of ZnO NPs at ca. 365 nm while the whole absorption range up to 700 nm indicates the absorption of the polymer-fullerene active layer. The AFM height image (FIG. 9b) shows the polymer BHJ after casting the active layer. As is apparent, the active layer filled the porous structure of the ZnO film. This resulted in a decrease in RMS roughness of the surface from 14.2 to 8.2 nm of the ZnO/PAA film before and after coating with the active layer, respectively. Although the pores are mostly filled with the active layer, the decrease in surface roughness is as not dramatic as in work (described above) with PbS quantum dots (QDs) in which the surface roughness of a 61-nm thick ZnO layer decreased from 18.8 to 1.5 nm upon coating with PbS QDs..sup.[36] This smaller decrease is likely due to the fact that the polymer chains are soft and will follow the surface architecture of the rough ZnO underneath.

[0109] FIG. 10a shows the efficiency of the as-prepared and annealed films as a function of the number of bilayers (n). The efficiency results show a strong dependence on the number of bilayers, until a plateau is reached at 4 bilayers. A further increase in the number of bilayers does not induce further efficiency improvements. Interestingly, as-prepared ETLs yield PCE values that are approximately a factor of two greater than those of thermally annealed films treated under atmospheric conditions. As shown in Table 3, as-prepared ETL solar cells achieved high PCEs of ca. 5.6% (Max.: 6%) with four bilayers of ZnO/PAA deposited by LbL with a thickness of 25 nm. These devices combined a FF of 55% and comparably high J.sub.sc of more than 12 mA cm.sup.−2. Meanwhile, solar cell devices with thermally annealed ETLs at 60, 80, 100, 200, and 300° C. (in a nitrogen atmosphere inside a glovebox) with the same number of bilayers achieved lower V.sub.oc, J.sub.sc, and FF than those of the as-prepared ETLs. This result indicates that annealing is not required for ETLs prepared by LbL and that in this case annealing does not help to improve device efficiency.

[0110] FIG. 10b shows the efficiencies of devices using as-prepared LbL and sputtered ETLs as a function of film thickness. Sputtered ETLs have a slightly higher efficiency than LbL films at lower thicknesses, whereas LbL ETLs yield higher efficiencies at higher thicknesses. Table 4 summarizes the device results with ZnO-sputtered interlayers. In fact, the maximum performance achieved with an optimized sputtered thickness of 10 nm is PCE of ca. 4.6% (Max.: 5.1%). This lower performance compared with the LbL deposition mainly comes from a lower FF, which could arise from the difference in the interfacial contact with the active layer, considering that the surface roughness of a sputtered ZnO film is about 2 nm. The current density-voltage (J-V) curves and the external quantum efficiency (EQE) spectra of optimized LbL and sputtered ETL-deposited devices are shown in FIGS. 10c and 10d, respectively. The EQE response is the highest in the range of 350-650 nm, consistent with the distinct onsets of absorption of the polymers, which are within 65-70%; this observation is in agreement with the device J.sub.sc values obtained (>12 mA cm.sup.−2). Furthermore, the EQE integration of the best device using sputtered ZnO and solution-processed LBL ZnO/PAA have values of 12.0 vs 11.8 mA/cm.sup.2, respectively, which are close to the average Jsc obtained on the J-V curve (11.9±0.3 and 12.1±0.4 mA cm.sup.−2, respectively). The higher PCE of the solution-processed ZnO/PAA comes essentially from the higher fill factor with respect to the sputtered ZnO (54±1 vs 46±3) and the slightly higher Voc (0.86±0.1 vs 0.84±0.1 V). This indicates that the estimated PCE of the devices are reliable. In FIG. 10d, a small difference in the absorption feature between the ZnO/PAA ETLs prepared by the LbL technique and that prepared by the sputtering technique was observed in the UV region. It was considered that the spectral mismatch is due to the absorption of different amounts of ZnO nanoparticles in the ZnO ETL prepared by the two techniques..sup.[36]

[0111] Thermal annealing of ZnO ETL in air or in a glovebox resulted in lowering the solar cell efficiency as seen in FIG. 10a. To understand the underlying reasons, the inventors conducted X-ray photoelectron spectroscopy (XPS) and attenuated total reflection Fourier-Transform Infrared (ATR-FTIR) experiments on the ZnO/PAA thin films before and after annealing in air. No change in the band gap of the ZnO NP was observed upon annealing. In addition, AFM height images did not exhibit a pronounced morphology or surface roughness change before and after annealing.

[0112] XPS C1s spectra (FIG. 11a) show that the ZnO/PAA film has about 10% less overall carbon content after annealing. It should be noted that the degradation of PAA has been reported to start partially (˜7%) at 300° C..sup.[45] It is well known that steady-state infrared experiments can give insights into the local interactions between donor and acceptor moieties..sup.[46] FIG. 11b shows clearly that the carboxylate group is broadened (due to charge delocalization) and downshifted by about 11 cm.sup.−1 after annealing, providing a clear signature for the electrostatic binding of the free carboxylate to the surface of ZnO NPs. Here, it was inferred that before annealing, these free carboxylates with their negative charges drive the electrons to the ZnO surface by means of repulsion forces. After annealing, conformational changes take place in the polyelectrolyte chain, and some of the free carboxylates bind electrostatically to the ZnO surface as indicated in the IR data, thus decreasing the effective repulsion force to drive the electrons to the surface of the ZnO layer. In addition, because of the binding mode and the conformational changes in the polyelectrolyte chain, it can be assumed that some of the active sites on the surface of the ZnO NP are no longer available as a pathway for the electrons to percolate. Electrostatic binding of free carboxylate together with the increased oxygen defects after annealing in air could contribute to the decreased device efficiency of the corresponding devices. It is worth pointing out that the device efficiency is also lower after annealing in a nitrogen environment compared to that of the as-prepared film, but higher than that of the air-annealed film, indicating that oxygen defects created after annealing in air can be considered as a major source of trap states, resulting in the low conversion efficiency after annealing.

[0113] In conclusion, the inventors have shown that the layer-by-layer assembly of ZnO NPs and polyacrylic acid (PAA) under ambient conditions is a simple and effective approach to produce efficient inverted BHJ polymer solar cells. Following this approach, the inventors demonstrated devices with ca. 6.0% PCE, exceeding the PCE values of devices with ZnO interlayers deposited via conventional sputtering methods. Depositing ZnO interlayers by the LbL approach is advantageous over other methods because it does not require any post-processing thermal annealing step and, in turn, it is applicable to flexible devices. In addition, the use of aqueous solvents minimizes the environmental footprint of the deposition process. The LbL-deposited ZnO/PAA platform is expected to be applicable to any inverted polymer-fullerene BHJ device as well as to other solar-cell architectures.

Experimental Section (Working Examples)

[0114] Preparation of ZnO ETL. The solar cells were prepared on glass substrates with tin-doped indium oxide (ITO, 15 Ωsq.sup.−1) patterned on the surface. The substrates were first immersed in an ultrasonic bath of diluted Extran 300 for 15 min, then rinsed in flowing deionized water for 5 min before being sonicated for 15 min in 0.1 M NaOH solution and rinsed with ultrapure water. This was followed by sonication in successive baths of isopropanol and acetone for 15 minutes each. Finally, the substrates were dried with pressurized nitrogen. Next, 0.5 g/L solutions of polyallylamine hydrochloride (PAH) (15000 g/mol) and polyacrylic acid (PAA) (15000 g/mol, 35% as sodium salt in water) were prepared in ultrapure water with the addition of 0.1 M NaCl. The ZnO NP dispersion (stabilized by cationic surfactant 3-Aminopropyl triethoxysilane, 50 wt.% in water, size<100 nm) was diluted at a concentration of 0.1 wt. % in ultrapure water. All chemicals were purchased from Sigma-Aldrich. For the LbL coating, substrates were first immersed for 20 minutes in PAH solution in order to coat one PAH layer to facilitate adsorption of the negatively charged PAA. The LbL coating was followed by immersion of substrates for 10 minutes in PAA and ZnO dispersions and consequently with three rinsing steps in ultrapure water for 2 minutes each. Finally, the films were dried with nitrogen after completion of the immersion cycles.

[0115] Characterization. The size of ZnO NPs was determined from TEM imaging. Thicknesses and refractive indices of thin films were measured by a spectroscopic ellipsometer (M2000, J. A. Wollam Co. Inc.) at variable incidence angles of 55-65° with increments of 5°. The thicknesses and refractive indices were calculated by fitting the data to a Cauchy model..sup.[47] AFM images were recorded (Dimension Icon microscope, Veeco) in the tapping mode under ambient conditions. Additionally, the thicknesses of the thin films were measured by AFM step analysis. Absorption spectra were recorded by a Cary5000 spectrometer (Agilent Technologies). XPS studies were carried out in a Kratos Axis Ultra DLD spectrometer equipped with a monochromatic Al Kα X-ray source (1486.6 eV) operating at 150 W, a multi-channel plate and delay line detector under a 1.0×10.sup.−9 Torr vacuum. Binding energies were referenced to the C1s binding energy of adventitious carbon contamination, which was taken to be 284.8 eV. ATR-FTIR spectra were recorded on an FTIR spectrometer (Thermo iS10), reflectance cell from (HARRICK VariGATR).

[0116] Device Fabrication. All active layer solutions were prepared in a glovebox using PBDTTPD and PC.sub.71BM purchased from SOLENNE. PBDTTPD and PC.sub.71BM were dissolved in chlorobenzene (containing 5% (v/v) of 1-chloronaphthalene (CN) additive) and the solutions were stirred overnight at 110° C. Optimized devices were prepared using a PBDTTPD:PC.sub.71BM in a ratio of 1:1.5 (by weight), with a concentration of 20 mg mL.sup.−1. The effects of various solvents, solution concentrations, additive concentrations, and blend ratios on device performance were examined.

[0117] The active layers were spin-cast from the solutions at 90° C. at an optimized speed for 45 s, using a programmable spin coater from Specialty Coating Systems (Model G3P-8), resulting in a film thickness of 100 to 120 nm. The samples were then dried at room temperature for 1 hour. Next, the samples were placed in a thermal evaporator to evaporate the 4 nm thick molybdenum oxide at 0.5 Å s.sup.−1 and the 80 nm thick silver electrodes at 3 Å s.sup.−1, at a pressure less than 1×10.sup.−7 Torr. Following electrode deposition, the samples underwent J-V testing.

[0118] J-V measurements of solar cells were performed in a glovebox with a Keithley 2400 source meter and an Oriel Sol3A Class AAA solar simulator calibrated to 1 sun, AM1.5 G, with a KG-5 silicon reference cell certified by Newport. The external quantum efficiency (EQE) measurements were performed at zero bias by illuminating the device with monochromatic light supplied from a Xenon arc lamp in combination with a dual-grating monochromator. The number of photons incident on the sample was calculated for each wavelength by using a silicon photodiode calibrated by NIST.

TABLE-US-00003 TABLE 3 PV Performance of the PBDTTPD in inverted BHJ Devices with PC.sub.71BM and LbL ZnO/PAA ETL after light soaking. J.sub.SC V.sub.OC FF Avg. PCE Max PCE Annealing [mA/cm.sup.2] [V] [%] [%] [%] None 12.1 ± 0.4 0.86 ± 0.1 54 ± 1 5.6 6.0  60° C./1 h 11.2 ± 0.3 0.83 ± 0.1 46 ± 3 4.3 4.7  80° C./1 h 12.0 ± 0.2 0.74 ± 0.1 39 ± 3 3.4 3.6 100° C./1 h 11.6 ± 0.3 0.64 ± 0.1 40 ± 4 3 3.4 200° C./1 h 11.3 ± 0.5 0.77 ± 0.1 49 ± 4 4.3 4.7 300° C./1 h 11.1 ± 0.4 0.81 ± 0.1 53 ± 3 4.8 5.3

TABLE-US-00004 TABLE 4 PV Performance of the PBDTTPD in inverted BHJ Devices with PC.sub.71BM and sputtered ZnO after light soaking. ZnO sputtered thickness J.sub.SC V.sub.OC FF Avg. PCE Max PCE [nm] [mA/cm.sup.2] [V] [%] [%] [%] 5 11.9 ± 0.4 0.78 ± 0.1 44 ± 5 4.1 4.8 10 11.9 ± 0.3 0.84 ± 0.1 46 ± 3 4.6 5.1 15 11.7 ± 0.3 0.82 ± 0.1 42 ± 4 4.0 4.6 20 11.3 ± 0.5 0.82 ± 0.1 46 ± 4 4.2 4.9

REFERENCES 1-47

[0119] [1] B. O'Regan, M. Gratzel, Nature 1991, 353, 737. [0120] [2] K. Ramanathan, M. A. Contreras, C. L. Perkins, S. Asher, F. S. Hasoon, J. Keane, D. Young, M. Romero, W. Metzger, R. Noufi, J. S. Ward, A. Duda, Prog. Photovoltaics: Res. Appl. 2003,11, 225. [0121] [3] K. L. Chopra, P. D. Paulson, V. Dutta, Prog. Photovoltaics: Res. Appl. 2004, 12, 69. [0122] [4] F. Fthenakis, J. E. Mason, K. Zweibel, Energy Policy 2009, 37, 387. [0123] [5] I. Repins, M. A. Contreras, B. Egaas, C. DeHart, J. Scharf, C. L. Perkins, B. To, R. Noufi, Prog. Photovoltaics: Res. Appl. 2008,16, 235. [0124] [6] A. Hagfeldt, M. Gratzel, Acc. Chem. Res. 2000, 33, 269. [0125] [7] A. Hagfeldt, G. Boschloo, L. Sun, L. Kloo, H. Pettersson, Chem. Rev. 2010, 110, 6595. [0126] [8] F. Odobel, Y. Pellegrin, J. Warnan, Energy Environ. Sci. 2013, 6, 2041. [0127] [9] H. Hoppe, N. S. Sariciftci, In Photoresponsive Polymers II; S. R. Marder, K.-S. Lee (Eds.); Springer Berlin Heidelberg: 2008; Vol. 214, p 1. [0128] [10] G. Li, R. Zhu, Y. Yang, Nat. Photon. 2012, 6, 153. [0129] [11] A. Kongkanand, K. Tvrdy, K. Takechi, M. Kuno, P. V. Kamat, J. Am. Chem. Soc. 2007, 130, 4007. [0130] [12] P. V. Kamat, J. Phys. Chem. C 2008, 112, 18737. [0131] [13] A. O. El-Ballouli, E. Alarousu, M. Bernardi, S. M. Aly, A. P. Lagrow, O. M. Bakr, O. F. Mohammed, J. Am. Chem. Soc. 2014,136, 6952. [0132] [14] J. Bouclé, H. J. Snaith, N. C. Greenham, J. Phys. Chem. C 2010, 114, 3664. [0133] [15] W. J. E. Beek, M. M. Wienk, R. A. J. Janssen, Adv. Mater. 2004, 16, 1009. [0134] [16] J. A. Anta, E. Guillen, R. Tena-Zaera, J. Phys. Chem. C 2012, 116, 11413. [0135] [17] G. Li, V. Shrotriya, J. Huang, Y. Yao, T. Moriarty, K. Emery, Y. Yang, Nat. Mater. 2005, 4, 864. [0136] [18] J. Y. Kim, K. Lee, N. E. Coates, D. Moses, T.-Q. Nguyen, M. Dante, A. J. Heeger, Science 2007, 317, 222. [0137] [19] Y. Liang, Z. Xu, J. Xia, S.-T. Tsai, Y. Wu, G. Li, C. Ray, L. Yu, Adv. Mater. 2010, 22, E135. [0138] [20] J. You, L. Dou, K. Yoshimura, T. Kato, K. Ohya, T. Moriarty, K. Emery, C.-C. Chen, J. Gao, G. Li, Y. Yang, Nat. Commun. 2013, 4, 1446. [0139] [21] W. U. Huynh, J. J. Dittmer, A. P. Alivisatos, Science 2002, 295, 2425. [0140] [22] A. M. Peiro, P. Ravirajan, K. Govender, D. S. Boyle, P. O'Brien, D. D. C. Bradley, J. Nelson, J. R. Durrant, J. Mater. Chem. 2006,16, 2088. [0141] [23] M. M. Lee, J. Teuscher, T. Miyasaka, T. N. Murakami, H. J. Snaith, Science 2012, 338, 643. [0142] [24] M. A. Loi, J. C. Hummelen, Nat. Mater. 2013, 12, 1087. [0143] [25] S. Schumann, R. D. Campo, B. Illy, A. C. Cruickshank, M. A. McLachlan, M. P. Ryan, D. J. Riley, D. W. McComb, T. S. Jones, J. Mater. Chem. 2011, 21, 2381. [0144] [26] Y. Sun, J. H. Seo, C. J. Takacs, J. Seifter, A. J. Heeger, Adv. Mater. 2011, 23, 1679. [0145] [27] H.-Y. Park, D. Lim, K.-D. Kim, S.-Y. Jang, J. Mater. Chem. A 2013, 1, 6327. [0146] [28] Y. Gao, I. Gereige, A. E. Labban, D. Cha, T. T. Isimjan, P. M. Beaujuge, ACS Appl. Mater. Interfaces 2014, 6, 2219. [0147] [29] H. Cheun, C. Fuentes-Hernandez, Y. Zhou, W. J. Potscavage Jr., S.-J. Kim, J. Shim, A. Dindar, B. Kippelen, J. Phys. Chem. C 2010, 114, 20713. [0148] [30] S. K. Hau, H.-L. Yip, N. S. Baek, J. Zou, K. O'Malley, A. K.-Y. Jen, Appl. Phys. Lett. 2008, 92, 253301. [0149] [31] Y.-J. Kang, K. Lim, S. Jung, D.-G. Kim, J.-K. Kim, C.-S. Kim, S. H. Kim, J.-W. Kang, Sol. Energy Mater. Sol. Cells 2012, 96, 137. [0150] [32] Z. Liang, Q. Zhang, O. Wiranwetchayan, J. Xi, Z. Yang, K. Park, C. Li, G. Cao, Adv. Funct. Mater. 2012, 22, 2194. [0151] [33] D. C. Lim, W. H. Shim, K.-D. Kim, H. O. Seo, J.-H. Lim, Y. Jeong, Y. D. Kim, K. H. Lee, Sol. Energy Mater. Sol. Cells 2011, 95, 3036. [0152] [34] L. K. Jagadamma, M. Abdelsamie, A. E. Labban, E. Aresu, G. O. N. Ndjawa, D. H. Anjum, D. Cha, P. M. Beaujuge, A. Amassian, J. Mater. Chem. A 2014, 2, 13321. [0153] [35] D. Liu, T. L. Kelly, Nat. Photon. 2013, 8,133. [0154] [36] M. Eita, A. Usman, A. O. El-Ballouli, E. Alarousu, O. M. Bah, O. F. Mohammed, Small 2014. DOI: 10.1002/sm11.201400939. [0155] [37] C. Piliego, T. W. Holcombe, J. D. Douglas, C. H. Woo, P. M. Beaujuge, J. M. J. Fréchet, J. Am. Chem. Soc. 2010, 132, 7595. [0156] [38] C. Cabanetos, A. E. Labban, J. A. Bartelt, J. D. Douglas, W. R. Mateker, J. M. J. Fréchet, M. D. McGehee, P. M. Beaujuge, J. Am. Chem. Soc. 2013, 135, 4656. [0157] [39] J. A. Bartelt, J. D. Douglas, W. R. Mateker, A. E. Labban, C. J. Tassone, M. F. Toney, J. M. J. Fréchet, P. M. Beaujuge, M. D. McGehee, Adv. Energy Mater. 2014, 1301733. [0158] [40] J. Warnan, C. Cabanetos, R. Bude, A. E. Labban, L. Li, P. M. Beaujuge, Chem. Mater. 2014, 26, 2829. [0159] [41] J. Warnan, A. E. Labban, C. Cabanetos, E. T. Hoke, P. K. Shukla, C. Risko, J.-L. Brédas, M. D. McGehee, P. M. Beaujuge, Chem. Mater. 2014, 26, 2299. [0160] [42] J. Warnan, C. Cabanetos, A. E. Labban, M. R. Hansen, C. Tassone, M. F. Toney, P. M. Beaujuge, Adv. Mater. 2014, 26, DOI: 10.1002/adma.201305344. [0161] (43) K. R. Graham, C. Cabanetos, J. P. Jahnke, M. N. Idso, A. E. Labban, G. O. N. Ndjawa, T. Heumueller, K. Vandewal, A. Salleo, B. F. Chmelka, A. Amassian, P. M. Beaujuge, M. D. McGehee, J. Am. Chem. Soc. 2014, 136, DOI: 10.1021/ja502985g. [0162] [44] M. Eita, L. Wägberg, M. Muhammed, J. Phys. Chem. C 2012, 116, 4621. [0163] [45] I. C. McNeill, S. M. T. Sadeghi, Polym. Degrad. Stab. 1990, 29, 233. [0164] [46] M. J. Tan, S. Zhong, J. Li, Z. Chen, W. Chen, ACS Appl. Mater. Interfaces 2013, 5, 4696. [0165] [47] H. G. Tompkins, E. A. Irene, Handbook of Ellipsometry, William Andrew Publishing, 2005.