Exciton Dissociation at Metal-Organic Interface and

Slides:



Advertisements
Similar presentations
BASIC SOLAR CELL TESTING Basic Structure of a Solar Cell.
Advertisements

Modeling in Electrochemical Engineering
Applications of Photovoltaic Technologies. 2 Solar cell structure How a solar cell should look like ?  It depends on the function it should perform,
COST Action MP0805 Meeting, Istanbul, April 12-13, 2010 University of Nottingham, UK Effects of Hydrogen Irradiation on Deep Levels in MBE Grown Dilute.
「 Quantum dot solar cells 」 A. J. Nozik, Physica E 14 (2002) YOSHIDA Lab. Hiroaki KAMIOKA.
Wei E.I. Sha, Wallace C.H. Choy, and Weng Cho Chew
Comprehensive Study of Plasmonic Effects in Organic Solar Cells Slide 1 Progress In Electromagnetics Research Symposium | August 12-15, 2013 | Stockholm,
SOLAR CELL TESTING. SOLAR CELL TESTING Basic Structure of a Solar Cell.
SOLAR CELL TESTING Basic Structure of a Solar Cell.
Figure 2.1 The p-n junction diode showing metal anode and cathode contacts connected to semiconductor p-type and n-type regions respectively. There are.
Coupled optoelectronic simulation of organic bulk-heterojunction solar cells: Parameter extraction and sensitivity analysis R. Häusermann,1,a E. Knapp,1.
Photodetector.
EE580 – Solar Cells Todd J. Kaiser
Characterisation and Reliability testing of THz Schottky diodes. By Chris Price Supervisor: Dr Byron Alderman December 2006 Preliminary.
Applications of Photovoltaic Technologies
Characterisation and Reliability Testing of THz Schottky Diodes Chris Price University of Birmingham, UK
Department of Electrical & Electronics Engineering ELE 1001: Basic Electrical Technology Lecture 5 Inductor.
Fei Yu and Vikram Kuppa School of Energy, Environmental, Biological and Medical Engineering College of Engineering and Applied Science University of Cincinnati.
Cells, Modules, and Arrays
Solar Cells Outline. Single-Junction Solar Cells. Multi-Junction Solar Cells.
Lesson 24: Photocell Electrical Characteristic and Circuit Model ET 332a Dc Motors, Generators and Energy Conversion Devices 1Lesson a.pptx.
C ARBON N ANOTUBE B ASED O RGANIC S OLAR C ELLS Arun Tej M. PhD Student EE Dept. and SCDT.
Photovoltaics: What material is best for your needs Benjamin Glassy Mark Ziffer 6/6/2013.
Characterization of organic bulk heterojunction and silicon nanowire solar cells Katherine Song Department of Electrical Engineering, Princeton University,
Electromagnetism Topics Covered in Chapter 14: 14-1: Ampere-turns of Magnetomotive Force (mmf) 14-2: Field Intensity (H) 14-3: B-H Magnetization Curve.
The educational-oriented pack of computer programs to simulate solar cell behavior Aleksy Patryn 1 Stanisław M. Pietruszko 2  Faculty of Electronics,
THE OPTIMUM PERFORMANCE OF POLYMER SOLAR CELLS By, N. Ibrahim2 M. O. Sid-Ahmed1 1 Sudan University of Science and Technology, Faculty of Science, Physics.
Figure 6 Voltage transient curve In fig.6, it is obvious that there is a significant voltage drop and transient at 1400s even though the load is not changed.
Integrated Circuit Devices Professor Ali Javey Summer 2009 MS Junctions Reading: Chapter14.
CHAPTER TWO THE PHOTOVOLTAIC EFFECT 2e A G.I. Module Energie Solaire Copyright, 2006 © Ahmed S. Bouazzi المدرسة الوطنية للمهندسين بتونس.
PowerPoint ® Presentation Chapter 5 Cells, Modules, and Arrays Photovoltaic Cells Current–Voltage (I–V) Curves PV Device Response Modules and Arrays.
Current Electricity Parallel CircuitSeries Circuit.
EXAMPLE 12.1 OBJECTIVE Solution Comment
Mapping free carrier diffusion in GaAs with radiative and heat- generating recombination Tim Gfroerer and Ryan Crum Davidson College, Davidson, NC with.
Current Electricity Parallel CircuitSeries Circuit.
Dr. Nicolae Atodiresei (Molecular Electronics & Spintronics Subgroup in the Peter Grünberg Institut and Institute for Advanced Simulation, Jülich, Germany.)
Influence of carrier mobility and interface trap states on the transfer characteristics of organic thin film transistors. INFM A. Bolognesi, A. Di Carlo.
Electricity 2 Thomas Edison Lesson Objectives I know some circuit symbols for common components. I know what is meant by resistance I know.
Fabrication and characterisation of high efficiency carbon nanotube based organic solar cells Lesias M Kotane NECSA-Wits workshop on Radiation, Material.
Modeling of an interface between two solids Ashcroft and Mermin Ch. 18 Sze Ch Review Chapter by Tersoff.
A Method to Rapidly Predict the Injection Rate in Dye Sensitized Solar Cells. Daniel R. Jones and Alessandro Troisi Department of Chemistry and Centre.
Photoluminescence and Photocurrent in a Blue LED Ben Stroup & Timothy Gfroerer, Davidson College, Davidson, NC Yong Zhang, University of North Carolina.
BASIC SOLAR CELL TESTING Basic Structure of a Solar Cell.
Presented by:- Nayanee Singh B.Tech(E.C.), 5 th sem Roll no: Banasthali University Rajasthan.
البحث الثامن بحث منفرد منشور فى مؤتمر دولى متخصص ( منشور التحكيم علي البحث الكامل ) Adel A. Elbaset 14 th International Middle East Power Systems Conference.
Organic solar cells based on CuPc and C 60 B. Delgertsetseg, G. Erdene-Ochir, R. Galbadrakh, D. Dorj and C. Ganzorig Department of Chemical Technology,
Cd(s) ↔ Cd2+ + 2e- depends on [Cd2+]s and not [Cd2+]o
Multiple choise questions related to lecture PV2
PN-junction diodes: Applications
SOLAR CELL TESTING. SOLAR CELL TESTING Basic Structure of a Solar Cell.
J. Appl. Phys. 112, (2012); Scanning Tunneling Microscopy/Spectroscopy Studies of Resistive Switching in Nb-doped.
DESIGN AND SIMULATION OF GRID CONNECTED
Optoelectronic Devices
Static electricity: define
Deep Level Transient Spectroscopy (DLTS)
BASIC SOLAR CELL TESTING
Carbon Nanotube Diode Design
Electron transfer in heterogeneous systems (on electrodes)
Department of Physics, Fudan University, Shanghai, China
Effect of Cryogenic Temperature Deposition of Various Metal Contacts to Bulk, Single-Crystal n-type ZnO J. Wright1, L. Stafford1, B.P. Gila1, D.P. Norton1,
Size dependent surface potential studies on Si and GeSi quantum dots
Taras Patlatiuk Zumbühl Group.
Electronic PRINCIPLES
Electron transfer in heterogeneous systems (on electrodes)
2. SEM images of different SiNW structures 3.Results and discussion
Multi-Exciton Generation and Solar Cell Physics
Triplet Sensitization by Lead Halide Perovskite Thin Films for Efficient Solid-State Photon Upconversion at Subsolar Fluxes  Sarah Wieghold, Alexander.
Unusual band-gap and band-edge bowing of SnxGe1-x
Chapter 3 Solid-State Diodes and Diode Circuits
Presentation transcript:

Exciton Dissociation at Metal-Organic Interface and The induced Surface Loss in BHJ Solar Cells Wenchao Yang, Deli Li and Chang-Qin Wu Department of Physics, Fudan University, Shanghai, 200433, PRC The pursuit of new energy resources that is clean and renewable is always a hot topic of research. Organic solar cells attracts very much attention due to their desirable properties like inexpensive, flexible over their inorganic counterparts. Bulkhetrojunction (BHJ) solar cell emerges as the most efficient and prominent type of organic solar cells in recent years. Experiments of transient photovoltage (TPV) find that there is possibly intensive exciton dissociation occurring at the anode (metal)-organic interface, which leads to an innegligible loss of free electrons, resulting the so-called surface loss. Starting from the device model and including the exciton dynamics as well, we calculate the J-V curves in different interfacial dissociation rates, and evaluate the magnitude of the surface loss and its influence to the short circuit current, open circuit voltage and the efficiency of the device. The role of bimolecular recombination is also investigated. Conclusions & References The short circuit current decreasing slightly with increasing of interfacial dissociation rate, until saturation at very large rate or small dissociation time. The decreasing of bulk dissociation rate can lead to the decreasing of short circuit current as well, and the effect is much more obvious . The open circuit voltage dose not change with the increasing of interfacial dissociation rate in Schottky contact device, while it decreases at Ohmic Contact one, this can be seen more clearly from the plot of net photocurrent versus the applied voltage. The interfacial dissociation proportion increases with the interfacial dissociation rate, varying conversely with the short circuit current. Its saturation can be understood with the help of exciton density profile. The excitons are equivalently quenched at the interface. The bimolecular recombination can reduce the interfacial dissociation proportion at high bias voltage in Ohmic contact device. [1] C. Deibel and V. Dyakonov, Rep. Prog. Phys. 73, 096401 (2010). [2] C. Deibel, T. Strobel, and V. Dyakonov, Phys. Rev. Lett. 103, 036402 (2009). [3] T. Strobel, C. Deibel and V. Dyakonov, Phys. Rev. Lett. 105, 266602 (2010).