Supporting Information

Similar documents
Solution-processable graphene nanomeshes with controlled

Electronic Supplementary Information (ESI)

Supporting Information. Benzophenone-based small molecular cathode interlayers with various polar groups for efficient polymer solar cells

Supporting Information The Roles of Alkyl Halide Additives in Enhancing Perovskite Solar Cell Performance

Supporting Information

Supporting Information

REDUCED GRAPHITE OXIDE-INDIUM TIN OXIDE COMPOSITES FOR TRANSPARENT ELECTRODE USING SOLUTION PROCESS

Improving Efficiency and Reproducibility of Perovskite Solar Cells through Aggregation Control in Polyelectrolytes Hole Transport Layer

Electronic Supplementary Information. inverted organic solar cells, towards mass production

4. CV curve of GQD on platinum electrode S9

Please do not adjust margins. New Approach for the Reduction of Graphene Oxide with Triphenylphosphine Dihalide

Supporting Information. Room temperature aqueous Sb 2 S 3 synthesis for inorganic-organic sensitized solar cells with efficiencies of up to 5.

Electronic Supplementary Information. Yunlong Guo, Chao Liu, Kento Inoue, Koji Harano, Hideyuki Tanaka,* and Eiichi Nakamura*

Shanghai Institute of Ceramics, Chinese Academy of Sciences, Dingxi, 1295, Changning,

Tailoring of Electron Collecting Oxide Nano-Particulate Layer for Flexible Perovskite Solar Cells. Gajeong-Ro, Yuseong-Gu, Daejeon , Korea

Graphene oxide was synthesized from graphite using the MH (modified Hummer s method) 30 and

An azafullerene acceptor for organic solar cells

Supporting Information

Direct measurements of exciton diffusion length limitations on organic solar cell performance

Department of Chemical Engineering, Pohang University of Science and Technology, San 31, Nam-gu, Pohang, Gyeongbuk , Republic of Korea.

Supporting information. and/or J -aggregation. Sergey V. Dayneko, Abby-Jo Payne and Gregory C. Welch*

SUPPORTING INFORMATION

Iodide-mediated room temperature reduction of graphene oxide: a rapid chemical route for the synthesis of a bifunctional electrocatalyst

Perovskite solar cells on metal substrate with high efficiency

High-Performance Semiconducting Polythiophenes for Organic Thin Film. Transistors by Beng S. Ong,* Yiliang Wu, Ping Liu and Sandra Gardner

Supporting Information

Supplementary Information

Electronic Supplementary Information. Au/Ag Core-shell Nanocuboids for High-efficiency Organic Solar Cells with Broadband Plasmonic Enhancement

Nanomaterials and Chemistry Key Laboratory, Wenzhou University, Wenzhou, (P. R. China).

Achieving high-performance planar perovskite solar cells with

Mixed Sn-Ge Perovskite for Enhanced Perovskite

A One-Step Low Temperature Processing Route for Organolead Halide Perovskite Solar Cells

Facile and purification-free synthesis of nitrogenated amphiphilic graphitic carbon dots

Electronic Supplementary Information

All-Inorganic CsPbI 2 Br Perovskite Solar Cells with High Efficiency. Exceeding 13%

Electronic Supplementary Information. Molecular Antenna Tailored Organic Thin-film Transistor for. Sensing Application

Efficient Grain Boundary Suture by Low-cost Tetra-ammonium Zinc Phthalocyanine for Stable Perovskite Solar Cells with Expanded Photo-response

Supporting Information for

Supporting Information

Controlled self-assembly of graphene oxide on a remote aluminum foil

Supporting Information

Supporting Information

Electronic Supplementary Information

Hysteresis-free low-temperature-processed planar perovskite solar cells with 19.1% efficiency

Electronic Supplementary Information

Enhancing Perovskite Solar Cell Performance by Interface Engineering Using CH 3 NH 3 PbBr 0.9 I 2.1 Quantum Dots

Multifunctional polyphosphazene-coated multi-walled carbon. nanotubes for the synergistic treatment of redox-responsive

Photocatalytic degradation of dyes over graphene-gold nanocomposites under visible light irradiation

Synergistic Improvements in Stability and Performance of Lead Iodide Perovskite Solar Cells Incorporating Salt Additives

Supporting information

Supporting Information

Cho Fai Jonathan Lau, Xiaofan Deng, Qingshan Ma, Jianghui Zheng, Jae S. Yun, Martin A.

Supporting Information

Severe Morphological Deformation of Spiro- Temperature

High-Performance Photocoupler Based on Perovskite Light Emitting Diode and Photodetector

Characterization of partially reduced graphene oxide as room

Mesoporous SnO 2 Single Crystals as an Effective Electron Collector for Perovskite Solar Cells

Supporting Information

Supplementary methods

Supporting Information

Probing the Kinetics of Ligand Exchange on Colloidal Gold. Nanoparticles by Surface-Enhanced Raman Scattering

Vertical Alignment of Reduced Graphene Oxide/Fe-oxide Hybrids Using the Magneto-Evaporation Method

Effects of Solubilizing Group Modification in Fullerene Bisadducts. on Normal and Inverted Type Polymer Solar Cells

Low-Bandgap Conjugated Polymers for High Efficient Photovoltaic. Yi-Chun Chen, Chao-Ying Yu, Yu-Ling Fan, Ling-I Hung, Chih-Ping Chen*, Ching

The photoluminescent graphene oxide serves as an acceptor rather. than a donor in the fluorescence resonance energy transfer pair of

Supporting Information

In a typical routine, the pristine CNT (purchased from Bill Nanotechnology, Inc.) were

Electronic Supplementary Information

Electronic Supplementary information (ESI) Nanodiamonds as Metal-Free Catalyst. 5 Few-Layer Graphene-Graphene Oxide Composite containing

Fabrication of graphene quantum dot-decorated graphene sheets via. chemical surface modification

The sacrificial role of graphene oxide in stabilising Fenton-like catalyst GO Fe 3 O 4

Functional p-type, polymerized organic. electrode interlayer in CH 3 NH 3 PbI 3. perovskite/fullerene planar heterojunction. hybrid solar cells

Supporting Information

High Performance Perovskite Solar Cells based on a PCBM:polystyrene blend electron transport layer

Electronic Supplementary Information

Aziridine in Polymers: A Strategy to Functionalize Polymers by Ring- Opening Reaction of Aziridine

Supporting Information

Supplementary information for:

Supporting Online Material for

Supporting Information

Processing and Properties of Highly Enriched Double-Walled. Carbon Nanotubes: Supplementary Information

One-pot Solvent-free Synthesis of Sodium Benzoate from the Oxidation of Benzyl Alcohol over Novel Efficient AuAg/TiO 2 Catalysts

Surfactant-free exfoliation of graphite in aqueous solutions

maximal photofluorescence decay time of 6 hours (purchased from Shenzhen HuiDuoSheng

Low-temperature-processed inorganic perovskite solar cells via solvent engineering with enhanced mass transport

Supplementary Material for. Zinc Oxide-Black Phosphorus Composites for Ultrasensitive Nitrogen

Synthesis of a highly conductive and large surface area graphene oxide hydrogel and its use in a supercapacitor

Supplementary Information. PCBM doped with fluorene-based polyelectrolytes as electron transporting layer for

Synthesis of 2 ) Structures by Small Molecule-Assisted Nucleation for Plasmon-Enhanced Photocatalytic Activity

Graphene oxide as acid catalyst for the room temperature. ring opening of epoxides

Laser Crystallization of Organic-Inorganic Hybrid

Anomalous high photovoltages observed in shish kebab-like organic p-n junction nanostructures

Correlating High Power Conversion Efficiency of PTB7:PC 71 BM

Carbon nanotube coated snowman-like particles and their electro-responsive characteristics. Ke Zhang, Ying Dan Liu and Hyoung Jin Choi

Fluorescent Bilayer Nanocoils from an Asymmetric Perylene Diimide with Ultrasensitivity for Amine Vapors

A Biosensor for the Detection of Single Base Mismatches in microrna

Nanoimprint-Transfer-Patterned Solids Enhance Light Absorption in Colloidal Quantum Dot Solar Cells

Supporting Information

Supplementary Figure 1 Detailed illustration on the fabrication process of templatestripped

Covalently Bound Clusters of Alpha-substituted PDI Rival Electron Acceptors to Fullerene for Organic Solar Cells

Transcription:

Electronic Supplementary Material (ESI) for ChemComm. This journal is The Royal Society of Chemistry 2015 Supporting Information Organic photovoltaic featuring graphene nanoribbons Seung Joo Lee, a Jae-Yeon Kim, a Hyeong Pil Kim, a Dongcheon Kim, a Wilson Jose da Silva,* b Fabio Kurt Schneider, b Abd. Rashid bin Mohd Yusoff, a and Jin Jang* a a Department of Information, Display and Advanced Display Research Center, Kyung Hee University, Dongdaemunku, Seoul 130-171, Republic of Korea. Fax: +82 2 961 9154; Tel: +82 2 961 0607; E-mail: jjang@khu.ac.kr b Universidade Tecnologica Federal do Parana, GPGEI Av. Sete de Setembro, 3165 CEP 80230-901 Curitiba, Parana, Brasil; Fax: +55 41 331 04691; Tel: +55 41 331 04691; E-mail: wjsilva2000@yahoo.com.br Experimental Section Synthesis of graphene nanoribbons (GNRs) and printing: The process for creating graphene nanoribbons is similar to that developed by the Tour group. 15,16 Using a 1 L Erlenmeyer flask with matching stopper, 35 mg of MWNTs was dispersed in 35 ml of concentrated H 2 SO 4 (99.999%, Sigma Aldrich) and stirred overnight. The MWNTs diameter ranger from 30 50 nm, and a length of 30 m, carbon purity is > 95%, and COOH functionalization is < 4%. Then 4 ml of H 3 PO 4 ( 99.999%, Sigma-Aldrich) was added to the mixture of carbon nanotubes and sulfuric acid (H 2 SO 4 :H 3 PO 4 final volume ratio of 9:1) and stirred for 15 min. Immediately thereafter, 0.34 g (8.5 wt equiv) of KMnO 4 ( 99%, Sigma Aldrich) was added to this mixture, and the reaction was heated at 65 C for 1 h. The reaction was stopped by placing the flask into an ice bath ( 200 ml) containing 3 ml of H 2 O 2 (30 wt % in H 2 O, Sigma Aldrich). The mixture was filtered over a 0.5 μm pore size poly(tetrafluoroethylene) (PTFE) membrane filter (Supelco) and then successively washed and filtered twice with 200 ml of 30% HCl (36.5-38%, 1 ppm chlorine free, Sigma Aldrich) and 200 ml of deionized water ( 98% HPLC, Sigma Aldrich). The resulting graphene oxide nanoribbons were first redispersed in 40 ml of deionized water by stirring overnight. They were then placed into SnakeSkin dialysis tubing (10 K molecular weight cutoff (MWCO), Fisher), dialyzed for 14 days to remove impurities from the inorganic acids and oxidized by a salt oxidizing mixture. Several steps of continuous sonication and ultracentrifugation were eliminated during the purification of the nanoribbons to avoid cutting the nanoribbons which would reduce the aspect ratio of the nanoribbons. After dialysis process, the suspension of graphene oxidized nanoribbons in water was filtered through a 0.5 μm pore size PTFE membrane filter. The solid obtained on the membrane filter was vacuum-dried overnight at room temperature to obtain approximately 24 mg of product along with the yield of about 70%. To reduce graphene oxide nanoribbons chemically, a 8 ml suspension of graphene oxide nanoribbons was dispersed in deionized water and was centrifuged (3000 rpm) for 30 min to provide a nanotube concentration of 3 mg/ml, which was then poured into a 100 ml two-neck round-bottom flask that was equipped with a stir bar, a reflux condenser, and a septum inlet containing 72 ml of anhydrous N,N-dimethylformamide (99.8%, Sigma-Aldrich). Then 4 μl of hydrazine monohydrate (N 2 H 4 ) (64-65%, Sigma-Aldrich) was added to the mixture and heated to 85 C for overnight reflux. The reaction was then cooled to room temperature and used directly to prepare the electrodes by inkjet printing. The inkjet ink was produced using two steps of filtration through the PTFE membrane (5 μm). Thermal reduction was performed in a 5 %

hydrogen/argon environment at 300 C for 2 h, and then the graphene nanoribbons were deposited onto the substrate. Ink preparation: An aqueous solution combining 1 mg/ml of graphene nanoribbons and 3 mg/ml of sodium n-dodecyl sulfate (SDS), an anionic surfactant was prepared and sonicated for 1 h. Then, the graphene nanoribbons ink was centrifuged at 10,000 rpm for 10 min and the supernatant was later removed. Finally, the supernatant was injected into a customized Autodrop pipette and printed using Autodrop Professional Positioning System AD-P-8000. Fabrication of solar cells: The glass was prepared using a cleaning process including detergent, acetone, and isopropyl alcohol with ultrasonication. Then, the glass was exposed to UV-ozone (20 min) to reform the surface. Inkjet printing technology was executed using an Autodrop printer (Microdrop, Norderstedt, Germany) to print the graphene nanoribbons on the glass substrate with a thickness of around 40 nm (dried at 50 C for 30 min). Then the PTB7:PC 71 BM BHJ active blend layer, with a nominal thickness of ~ 80 nm was prepared by spin-coating a mixed solvent of chlorobenzene/1,8-diiodoctane (97:3% by volume) solution (concentration, 25 mg ml -1 ) at 1000 rpm for 2 minutes. A 10 nm of C 60 -bis layer and a 100 nm of Ag layer were subsequently evaporated through a shadow mask to define the active area of the devices and form a top anode. The devices were encapsulated by a cleaned cover glass and a UV-curable epoxy in the N 2 -filled glove box. Measurement and characterization: After calibration of the light source using silicon reference cells with an AM 1.5 Global solar simulator, the encapsulated BHJ solar cells were measured during the exposure of the devices to an intensity of 100 mw/cm 2 using a Keithley 236 source unit. Then, the J V curves and PCE parameters (V OC, J SC, and FF) were obtained. To determine the exact cell areas, we used the aperture of 0.04 cm 2 on top of the deposited Al cathode while taking measurements. The morphology and surface roughness of BHJs with and without interlayers were determined by atomic-force microscopy (AFM; Veeco, USA; D3100) to confirm the contact of interlayers. The IPCEs were investigated by a QE measurement system (PV measurements, Inc.) after the calibration of monochromatic power density to check and match with the J V characteristics. For the UPS analysis, the PTB7:PC 71 BM BHJ was spin-casted onto the ITO-glass substrate. The films were dried at 80 C for 10 minutes. The UPS analysis chamber was equipped with a hemispherical electron-energy analyzer (Kratos Ultra Spectrometer), and was maintained at 1.33 x 10-7 Pa. UPS measurements were carried out using the He I (hv=21.2 ev) source. The electronenergy analyzer was operated at constant pass energy of 10 ev (for UPS). During UPS measurements, a sample bias of ~ 9 V was used in order to separate the sample and the secondary edge for the analyzer.

(a) (b) (b)

(c) (d)

(e) (f) Figure S1. UPS spectra of (a) GNRs, (b) CNTs, (c) PTB7:PC 71 BM, (d) PTB7:PC 71 BM/PEDOT:PSS, (e) PTB7:PC 71 BM/MoO 3 /GNRs, and (f)

PTB7:PC 71 BM/CNTs/GNRs layers. The blue color line is the reference substrate while the red color line is the real sample. The UPS spectra were obtained using HeI irradiation with hv=21.23 ev produced by a UV source. During UPS measurements the analyzer was working at the Constant Retarding Ratio (CRR), with CRR of 10. The work function was determined from the UPS spectra by subtracting their width from the HeI excitation energy. Figure S1 demonstrates the UPS spectra with different onset values. Transmittance (a.u.) C-O C=C C=O O-H (carboxyl) GNRs CNTs Coupling O-H 1000 2000 3000 4000 Wavenumber (cm -1 ) Figure S2. FTIR spectra of pristine CNTs and GNRs. Figure S2 demonstrates clear differences between the pristine CNT and pristine GNRs.

Figure S3. The zoom in HR-TEM image from Figure 3c. Figure S3 displays the zoom in HR-TEM image obtained from Figure 3c showing the zigzg configuration of our graphene nanoribbons.

Current Density (ma/cm 2 ) 100 10 1 0.1 0.01 No HTL PEDOT:PSS GNRs GNRs/MoO 3 GNRs/CNTs 1E-3 1E-4 1E-5 1E-6-4 -3-2 -1 0 1 Bias (V) Figure S4. Dark current-voltage plots of OPVs with various HTLs. Figure S4 shows the dark current-voltage plot of different OPVs with various HTLs.

70 60 50 EQE (%) 40 30 20 10 1 layer 2 layers 3 layers 0 300 400 500 600 700 800 Wavelength (nm) Figure S5. EQE spectra for OPVs with various GNRs. Figure S5 shows the EQE spectra for OPVs with various GNR layers. From this figure the highest EQE is from the OPV with 1 layer of GNRs.

Table S1. Photovoltaic parameters of GNRs-based organic photovoltaic with different HTLs. HTL J sc V oc FF PCE (ma/cm 2 ) (V) (%) (%) No HTL -11.20±0.11 0.70±0.01 51.05±0.10 4.00±0.03 PEDOT:PSS -16.18±0.10 0.76±0.01 59.56±0.11 7.32±0.04 CNTs -11.23±0.07 0.69±0.01 57.19±0.04 4.45±0.10 GNRs -13.74±0.02 0.74±0.01 56.14±0.02 5.88±0.10 GNRs/MoO 3-14.50±0.10 0.75±0.01 57.67±0.06 6.11±0.01 GNRs/CNTs -15.79±0.02 0.75±0.01 63.84±0.01 7.60±0.01 Table S2. Photovoltaic parameters of the fabricated device with different GNRs layers. GNRs J sc (ma/cm 2 ) V oc (V) FF (%) PCE (%) R s ( cm 2 ) 1 layer -15.79±0.02 0.75±0.01 63.84±0.01 7.60±0.01 14.22 2 layers -12.42±0.11 0.73±0.01 56.86±0.13 5.14±0.04 26.13 3 layers -11.20±0.02 0.70±0.01 56.68±0.11 4.44±0.11 26.04