Materials and Technologies for Making Perovskite-based Solar Cell DENG Sunbin 3/12/2014 1.

Slides:



Advertisements
Similar presentations
Nanomaterials and Synthesis
Advertisements

Nanowire dye-sensitized solar cells
Michael Grätzel, YouTube EPFL
Dye-Sensitized Solar Cells Цветосенсибилизиованные солнечные ячейки.
Structural Properties of Electron Beam Deposited CIGS Thin Films Author 1, Author 2, Author 3, Author 4 a Department of Electronics, Erode Arts College,
Juan Bisquert Nanostructured Energy Devices: Equilibrium Concepts and Kinetics CRC Press 1 1Introduction 2Electrostatic and thermodynamic potentials of.
Materials and Technologies for Making Perovskite-based Solar Cell
Silicon Nanowire based Solar Cells
1 Air Force Research Laboratory Dr. Michael F. Durstock, , Device Architectures.. Aluminum ITO Glass V Electron.
Fei Yu and Vikram Kuppa School of Energy, Environmental, Biological and Medical Engineering College of Engineering and Applied Science University of Cincinnati.
The Effect of Carbon Nanotubes in Polymer Photovoltaic Cells May 13, 2010 JESUS GUARDADO, LEAH NATION, HUY NGUYEN, TINA RO.
Synthesis of Metal Oxide Nanoparticles by Flame Method Synthesis of Metal Oxide Nanoparticles by Flame Method.
O RGANIC L IGHT E MITTING D IODES Andrew Sanders, Fawzi Salama, John P. Handrigan 12/02/2010.
Kiarash Kiantaj EEC235/Spring 2008
Preparation of Fluorine-doped Tin Oxide by a Spray Pyrolysis Deposition and Its Application to the Fabrication of Dye-sensitized Solar Cell Module S. Kaneko,
Nathan Duderstadt, Chemical Engineering, University of Cincinnati Stoney Sutton, Electrical Engineering, University of Cincinnati Kate Yoshino, Engineering.
Energy of the Future: Solar Cells Rade Kuljic 1, Hyeson Jung 1, Ayan Kar 1, Michael A. Stroscio 1,2 and Mitra Dutta 1,3 1 Department of Electrical and.
PREPARATION OF ZnO NANOWIRES BY ELECTROCHEMICAL DEPOSITION
VFET – A Transistor Structure for Amorphous semiconductors Michael Greenman, Ariel Ben-Sasson, Nir Tessler Sara and Moshe Zisapel Nano-Electronic Center,
Dye Sensitised Solar Cells
The Sixth International Workshop on Junction Technology (IWJT), May 15-16, 2006, Shanghai, China. Formation and characterization of aluminum-oxide by stack-
Electrical transport in ZnO and TiO 2 nanowires (for solar cell application) Chun-Chung Su and Chao-Cheng Kaun Advanced Computation & Modeling Group.
November 2004 Beta Iron Disilicide (  -FeSi 2 ) As an Environmentally Friendly Semiconductor for Space Use 1.Kankyo Semiconductors Co., Ltd. 2.Nippon.
Cebo. Ndlangamandla Synthesis of Iron Oxides nanorods for water splitting application Energy Postgraduate Conference 2013 iThemba LABS/ UniZulu.
IMPROVEMENT OF HEIGHT UNIFORMITY OF ZnO NANOWIRE ARRAYS BY USING ELECTROPOLISHING METHOD Nano-Scale Measurement & AnaLysis Lab.
J-V Characteristics Optical Properties Above-11%-Efficiency Organic–Inorganic Hybrid Solar Cells with Omnidirectional Harvesting Characteristics by Employing.
Polymer Photovoltaic Cells: Prototype Presentation April 15, 2010 JESUS GUARDADO, LEAH NATION, HUY NGUYEN, TINA RO.
(M): No Class (Memorial Day) 5.27 (W): Energy and Nanotechnology 5.28 (Th): LAB: Solar Cell (M): Project Presentations 6.03 (W): LAB: Antimicrobial.
U C L A Polymer Solar Cells A cost effective renewable energy solution for future – Earth abundant, non-toxic & manufacturing friendly – Light weight power.
April 27, O’Dwyer, C. et al. Bottom-up growth of fully transparent contact layers of indium tin oxide nanowires for light emitting devices. Nature.
Fabrication and characterisation of high efficiency carbon nanotube based organic solar cells Lesias M Kotane NECSA-Wits workshop on Radiation, Material.
DiffusjonDrift - + Diffusjon Drift. Solid State Electronic Devices, 7e, Global Edition Ben G. Streetman | Sanjay Kumar Banerjee Copyright © Pearson Education.
1 Institute of Isotopes, Budapest, Hungary; 2 Research Institute for Technical Physics and Materials Science, Budapest Hungary; 3 Chemical Physics of Materials,
1 Enhanced efficiency of GaN-based light-emitting diodes with periodic textured Ga-doped ZnO transparent contact layer 指導教授 : 管 鴻 (Hon Kuan) 老師 學生 : 李宗育.
M.S. Hossain, N.A. Khan, M. Akhtaruzzaman, A. R. M. Alamoud and N. Amin Solar Energy Research Institute (SERI) Universiti Kebangsaan Malaysia (UKM) Selangor,
Heterojunction Solar Cells Using Chemically co-doped Titania Nanotube Arrays for Simultaneous Light Absorption and Carrier Transport Hao Zeng, SUNY at.
Introduction to Thin Film CIGS Solar Cells
Presented by:- Nayanee Singh B.Tech(E.C.), 5 th sem Roll no: Banasthali University Rajasthan.
A bottom-up rationale for OPV architecture Fabrication Performance Challenges Research opportunities Research Methods in PV: Organic photovoltaic devices.
Date of download: 6/7/2016 Copyright © 2016 SPIE. All rights reserved. (a) Chemical structures of the interface dye (ID) D5L0A3 and hole transporting dye.
Hadi Maghsoudi 27 February 2015
Characterization of mixed films
Methodology Electrodeposited Pt and Pt/Ni electrodes for dye sensitized solar cells with improved stability G. Syrrokostas, G. Leftheriotis* and P. Yianoulis.
IN THE NAME OF GOD.
Hadi Maghsoudi 27 February 2015
THE EFFECT OF SPIN COATING RATE ON MICROSTRUCTURES OF CUPROUS OXIDE THIN FILM PREPARED BY SOL-GEL TECHNIQUE DEWI SURIYANI BT CHE HALIN School of Material.
III.Photoelectrochemical Performance Test
Centro de Investigación y de Estudios Avanzados del Institúto Politécnico Nacional (Cinvestav IPN) Palladium Nanoparticles Formation in Si Substrates from.
Volume 1, Issue 2, Pages (October 2017)
Volume 2, Issue 3, Pages (March 2017)
Volume 3, Issue 2, Pages (August 2017)
Interface Engineering
Azopolymer materials for optical recording
Volume 1, Issue 2, Pages (October 2017)
Volume 2, Issue 6, Pages (June 2017)
Nat. Rev. Mater. doi: /natrevmats
IRG-2: MAPLE of Polymer Films for Morphology Control (DMR ) Craig Arnold, Lynn Loo, Rodney Priestley, Princeton University Substrate (Si) crystal.
Ionic liquid gating of VO2 with a hBN interfacial barrier
Revolutionizing solar power with perovskites
Epitaxial Deposition
Rui Wang, Jintao Wang, Shaun Tan, Yu Duan, Zhao-Kui Wang, Yang Yang
Volume 1, Issue 2, Pages (October 2017)
Sawanta S. Mali, Jyoti V. Patil, Hyungjin Kim, Chang Kook Hong
In situ recombination junction between p-Si and TiO2 enables high-efficiency monolithic perovskite/Si tandem cells by Heping Shen, Stefan T. Omelchenko,
Illustration of MIS-C and the characterization of the device structure
by David P. McMeekin, Golnaz Sadoughi, Waqaas Rehman, Giles E
Main Text Figures.
Design and fabrication of a wafer-scale organic printed photonic chip
Fig. 3 Device architecture, photovoltaic performance, and operational stability of 3D/2D bilayer PSCs. Device architecture, photovoltaic performance, and.
Fabrication of SnS/SnS2 heterostructures
Presentation transcript:

Materials and Technologies for Making Perovskite-based Solar Cell DENG Sunbin 3/12/2014 1

2 Outline 1. Introduction 2. Materials for PSC Fabrication 3. Processes for PSC Fabrication 4. Potential Trend in the Future 5. Conclusion

3 Perovskite Solar Cell (PSC) —— A New Era Figure 1: Research cell efficiency records. This plot is courtesy of the National Renewable Energy Laboratory, Golden, CO.

4 Perovskite Materials in PSCs Figure 2: Cubic pervovskite crystal structure. For photovoltaically interesting perovskites, the larger organic cations occupy position A whereas metal cations and halides occupy the B and X positions, respectively.  Formula: ABX 3  Organometal halide (for photovoltaics) A  Organic cations (CH 3 NH 3 +, CH 3 CH 2 NH 3 +, NH 2 CH=NH 2 + ) B  Metal cations (Pb 2+, Sn 2+ ) X  Halides (I -, Br -, Cl - ) —— CH 3 NH 3 MX 3 (M=Pb, Sn; X=Cl, Br or I)  Some key attributes:  Ease of fabrication  Strong solar absorption  Low non-radiative carrier recombination  etc. Green M A, et al. Nature Photonics, 2014, 8(7):

5 Progress of Perovskite Solar Cell Fabrication  First stage: Material leading  Second stage: Process leading

6 Milestones  Dye: Others  Perovskite  3.8%, CH 3 NH 3 PbI 3 /CH 3 NH 3 PbBr 3 ( Kojima A, et al. J. Am. Chem. Soc., 2009, 131(17): )  Thinner and stronger sensitizer  Rapid degradation  HTM: Liquid electrolyte  Solid state  10.9%, CH 3 NH 3 PbI 3 / Spiro-MeOTAD ( Park N G, Gra ̈ tzel M, et al. Scientific reports, 2012, 2. )  9.7%, CH 3 NH 3 PbI 3-x Cl x / Spiro-MeOTAD ( Snaith H J, et al. Science, 2012, 338(6107): )  Enhanced stability, record-breaking efficiency, thinner  Mesoscopic scaffold layer: TiO 2  Al 2 O 3  10.9%, CH 3 NH 3 PbI 3 ( Park N G, Gra ̈ tzel M, et al. Scientific reports, 2012, 2. )  Electron transport property  HTM elimination  5.5%, TiO 2 /CH 3 NH 3 PbI 3 heterojunction ( Etgar L, et al. J. Am. Chem. Soc., 2012, 134(42): )  12.8%, TiO 2 /ZrO/(5-AVA) x (MA) 1-x PbI 3 ( Mei A, et al. Science, 2014, 345(6194): )  Hole transport property  Ambipolar semiconductor  Planar “p-i-n” heterojunction PSC: 15.4%, CH 3 NH 3 PbI 3-x Cl x ( Snaith H J, et al. Nature, 2013, 501(7467): ) Figure 3: Several notable milestones led by materials in the progress of PSC fabrication, resulting in the evolution of device structure.

7 (a) (b) (c) (d) PSC Structure Figure 4: Historic evolution of PSC structure, starting from (a) original mesoscopic DSSC, using the perovskite dye as a sensitizer, to currently (b) Meso-superstructured PSC (MSSC), employing a mesoscopic Al 2 O 3 scaffold layer with a conformal overlayer of the perovskite which plays as a light harvester and electron conductor; (c) PSC with mesoscopic TiO 2 scaffold infiltrated by the perovskite. The perovskite is a light harvester as well as hole conductor; (c) Planar p-i-n heterojunction PSC without mesoscopic metal oxide scaffold. The perovskite behaves as both ambipolar semiconductor and light harvester. Grätzel M. Nature materials, 2014, 13(9):

8 Deposition of the Perovskite  Solution process  One-step spin coating  Two-step (Sequential) deposition  Vapor process (for planar PSCs particularly)  Dual-source thermal evaporation  Sequential liquid-vapor phase deposition

9 One-step Spin Coating  A mixture of PbX 2 and CH 3 NH 3 X (X=Cl, Br, I) in a common solvent (DMF, GBL, DMSO, etc.)  Uncontrolled precipitation of the perovskite  Shapeless morphology  Poor reproducibility of photovoltaic performance Figure 5: Schematic illustration of one-step spin coating method.

10 Two-step (Sequential) Solution-Based Deposition i.Spin coat PbX 2 solution ii.Dip into CH 3 NH 3 X solution iii.CH 3 NH 3 PbX 3 film  Better morphology and interfaces  Increased light scattering due to large crystal size  Boosted photovoltaic performance (15%) and reproducibility Figure 6: Schematic illustration of sequential solution-based deposition method. Figure 7: The cross-section images of PSC fabricated by (a) the sequential spin coating process and (b) the conventional single-step spin coating process. Burschka J, et al. Nature, 2013, 499(7458):

11 Dual-Source High-Vacuum Thermal Evaporation (Planar)  Better morphology and uniformity of perovskite film  Better thickness control  15.4% (for planar CH 3 NH 3 PbI 3-x Cl x solar cell)  Compatible with traditional technologies (high vacuum)  Inorganic source PbX 2 + Organic source CH 3 NH 3 X  Co-evaporation at mbar  Annealing for crystallization Figure 8: (a) Scheme of dual-source thermal evaporation system. (b) Generic structure of a planar heterojunction p–i–n perovskite solar cell. (c) Current- density/voltage curves of vapor-deposited and solution-processed PSCs. Figure 9: Comparison of the perovskite film uniformity between vapor-deposition and solution-process methods. Snaith H J, et al. Nature, 2013, 501(7467):

12 Sequential Liquid-Vapor Phase Deposition (Planar)  Solution process (Inorganic PbX 2 )  Annealing at 150 °C  Vapor treatment (Organic CH 3 NH 3 X)  In situ reaction  Overcome high vacuum issue  Kinetic reactivity of CH 3 NH 3 X and thermodynamic stability of perovskite  Well-defined grain structure with grain sizes up to microscale  Full surface coverage & small surface roughness  12.1% (for planar CH 3 NH 3 PbI solar cell) Figure 10: Schematic illustration of perovskite film formation in the sequential liquid-vapor phase deposition. Figure 11: Perovskite film on the FTO/c-TiO 2 substrate, obtained by reacting PbI 2 film and CH 3 NH 3 I vapor at 150 °C for 2 h in N 2 atmosphere: (a) XRD pattern; (b) top-view SEM image (inset image with higher resolution, scale bar 1 μm); (c) tapping-mode AFM height images (5 × 5 μm); and (d) cross-sectional SEM image. Chen Q, et al. J. Am. Chem. Soc., 2013, 136(2):

13 Future Potential Technologies for PSC Fabrication  Low-temperature process  New ETM: TiO 2  ZnO Figure 12: (a) Schematic illustration of the hole- conductor-free, fully printable mesoscopic PSC. (b) Energy band diagram of this triple-layer PSC. Mei A, et al. Science, 2014, 345(6194):  Extra HTM free  Printing technology Figure 13: (a) Device architecture of the ITO/ZnO/CH 3 NH 3 PbI 3 /spiro-OMeTAD/Ag PSC. (b) Energy band diagram of the various device components. Liu D, et al. Nature Photonics, 2014, 8(2):  Interface Engineering  19.3% ! Zhou H, et al. Science, 2014, 345(6196): Figure 14: (a) SEM cross-sectional image of the device. The layers from the bottom are: (i) ITO/PEIE, (ii) Y-TiO 2, (iii) perovskite, (iv) spiro-OMeTAD, and (v) Au. (b) Diagram of energy levels (relative to the vacuum level) of each functional layer in the device.

14 Conclusion  Four material-leading milestones and three possible device structures for PSC fabrication are concluded.  In PSC fabrication, there are solution processes and vapor processes (for planar PSCs).  Sequential (two-step) solution-processed deposition could form better morphological perovskite layer than one-step spin coating deposition, resulting in better photovoltaic performance and reproducibility.  High-quality and controllable perovskite film could be deposited by vapor processes in planar PSC fabrication.  Emerging technologies such as low-temperature process and interface engineering may represent potential trend for PSC fabrication in the future.

15 Thank you!