( P ) Thales Photo-Electrochemical Techniques. Outline. Photo-Electrochemical Set-Up. Standard Solar Cell Measurements
|
|
- Jodie Knight
- 5 years ago
- Views:
Transcription
1 Outline Thales hoto-electrochemical Techniques Dynamic- and Spectral Methods for Measurements on DSSC, OSC, OLED and Electro-Chromic Devices C.-A. Schiller Standard Solar Cell Measurements Basics and the Applications of CMS/CMVS Additional dynamic techniques for Solar Cells Spectral resolved hotocurrent determination Optical Absorption / Extinction measurement in an electrochemical set-up Dynamic Transmittance / Reflectance measurement hoto-electrochemical Set-p Zennium Electrochemical orkstation Standard Solar Cell Measurements LED light source carrier with photosense amplifier and lluminator Cell under test Light source control potentiostat. (feedback control photosensor hidden behind the cell) Maximum Voltage, Current, ower, Fill Factor and CE of an OSC under blue illumination at /m². Force-response couples for ES, MVS and MS The Three Facts of a Solar Cell: Voltage Current-ntensity No information about the photoelectric process through ES Two additional force-response couples can be used for further transfer function analysis: Dynamic hotocurrent vs. ntensity MS Dynamic hotovoltage vs. ntensity MVS = a ( ) = a ( ) = a ( ) = Voltage across, = Current through the object. = llumination ntensity Anode p + n n + V A Cathode h ν cell current cell voltage Each transfer function emphasizes different parts of the system! ES MS MVS Z ( ω) =, [ ] = Ω Z ( ω) =, [ ] ( ω) =, [ ] A m = V m =
2 The Aim of MS / MVS when optimizing SC Comparison Between Conventional MS and CMS The competition between photo-charge recombination and charge diffusion affects the efficiency of OSC & DSSC. R i = MS R i = SC C SC ( ω) =, ( ) = ω, MS MVS = A m V m = Dynamic photocurrent vs. intensity MS: electron diffusion time constant τ c dominates at short-circuit under illumination. Dynamic photo-voltage vs. intensity MVS: electron recombination time constant τ r dominates at OC under illumination. The ratio - τ c / τ r determines the efficiency. Dynamic network analysis: join ES, MS & MVS results to find a common model. 7 Cell current ( ω) = LED current Cell voltage ( ω) = LED current Conventional MS: The LED control current is used as force signal information. The actual intensity and modulation is uncertain. Cell current Cell voltage ( ω ) = ( ) ω = ntensity ntensity CMS: The measured intensity is used as force signal information.the actual intensity is controlled with a photo-sensor at the site of the cell and regulated by means of an operational amplifier feedback circuit. MS & MVS on a ZnO-Based DSSC Analysis of the ZnO-Based DSSC MS & MVS Dynamic efficiency spectra measured on a ZnO based DSSC in Bode representation, on the left MS, on the right MVS Analysis of the dynamic efficiency spectra of a ZnO based DSSC in Nyquist representation. The circles indicate the measurement samples, the solid line curves the simulated spectra, modeling the electron diffusion and recombination time constants τ c and τ r,. On the left the MS with the breakpoint frequency /πτ c is depicted, on the right the MVS with /πτ r rinciple of a bulk hetero-junction type OSC OSC (Cr ( Cr-Al Al-Cr Cr-T T-CBM CBM-EDOT:SS EDOT:SS-Au) CMS / CMVS at Short Circuit Conditions photocurrent / µa - m phase / o photovoltage / V - m phase / o Donor Acceptor 7 7 Acceptor: CBM TO.7eV LMO.eV LMO.7eV Al.eV 7w w w m m m 7w w w Donor: T EDOT.eV OMO.eV OMO.eV K K K K K K m m K K K K
3 OSC mpedance Characteristics under Light Selected Dynamic Measurements on the OSC impedance / Ω phase / o impedance / Ω K 7 K K phase / o 7 Multiple Function Gradient calculation Complex Nonlinear Least Squares Fit ZCV arameter variation Measured spectra: Model Z: impedance C: photo-current ZCV(t,ω, n ) V: photo-voltage Deviations Z ( ω i ) Σ ( Z(ω i ) - ZCV(,ω i ) ) skalar deviation sum fit loop 7 7w_ocv w_ocv w_ocv K 7w w w C ( ω j ) Σ ( C(ω j ) - ZCV(,ω j ) ) V ( ω k ) Σ ( V(ω k ) - ZCV(,ω k ) ) Σ K K K K K at open circuit conditions K K K K K at short circuit conditions on the left: experimental results from ES, MS and MVS of the OSC. On the right: scheme of the Thales SM TRFT CNLS joined fitting procedure for three different kinds of spectral transfer functions: impedance, dynamic photocurrent and dynamic photo-voltage. Fit Results of the Dynamic Measurements on the OSC 7 Charge Extraction after N.. Duffy, L.M. eter et al N ser # hoto-active layer: hotocurrent source, breakpoint frequencies blocked hole diffusion in the porous layer electrostatic capacity olymer anode: finite length diffusion of holes in the anode layer electrostatic capacity Shunt loss shunt resistance Series loss 7 contact resistance. µa. Mz. Mz 7. KΩ s -/ 7.7 Ks -. nf. KΩ s -/. Ks -. nf. KΩ 7. Ω Assignment of the bulk hetero-junction OSC phases and processes to a dynamic equivalent circuit model Charge Extraction of a DSSC with different delay times between turning light off and start of discharging. The aim is the photo electron density distribution vs. potential hotocurrent Spectra: ncident hoton to Current Conversion Efficiency CE Typical CE of Alternative Solar Cells with Different orking rinciple Setup for CE measurements consisting of the Tunable Light Source with supply potentiostat and sample cell controlled by the Zahner Zennium 7 hotocurrent and CE measurements of two different DSSC and an OSC recorded with the Zahner tunable light source TLS
4 hoto-electrochemical Transmission / Absorption Measurements OSC and OLED orkfunction Vacuum Level TO p BG n Al TO p BG n Ca:Mg Setup for photo-electrochemical absorption/transmission measurements Band schemes of a typical OSC (bulk hetero-junction type, left) and an OLED (three layer type, right). p: hole transport layer (e.g. EDOT:SS), n: electron transport layer (e.g. left: CBM as - acceptor. right: Alq [tris(-hydroxyquinoline) aluminum]), BG: active band-gap material for photon absorption (left, e.g. T as -donor) respectively electron-hole recombination under light emission (right, e.g. r(ppy) = fac tris(-phenylpyridine) iridium). Extinction Spectra Series vs. Cell Voltage Referenced to Ag/AgCl AgCl. T-EDOT:SS EDOT:SS Film in Acetonitrile / TBA-F, under N., Absorption- and mpedance Spectra of an OSC / OLED olymer anion incorporation -.V +.7V hν hν -. V. +. V +. V extinction. +.7 V.. 7 wavelength / nm Extinction spectra series vs. cell voltage referenced to Ag/AgCl m-nacl of a T-EDOT:SS film in Acetonitrile / TBA-F (on the left) and the corresponding impedance spectra (on the right). Stability and Reversibility of the Film under Test Model Fit of the mpedance Spectra Series vs. Cell Voltage. extinction V at start -. V at end current / µa cycles mv/s +. mc -. mc impedance / Ω K K K +.7V +.V -.V phase / o 7 +.V +.7V -.V - m K K K K m K K K K. 7 wavelength / nm - potential / mv mpedance modulus (left) and phase angle diagram (right). Symbols: Experimental samples. Solid lines: Model Fit.
5 impedance'' / KΩ Model Fit of the mpedance Spectra Series. V 7 impedance' / KΩ -.V -.V ACN-TBA F Modeling & fit of the reduced state spectra (left) and the model used (right).,: inert hole transport layer with, porous distribution.,: active layer redox Faraday impedance, film assigned diffusion, 7 layer capacity with, porous distribution. T : electrolyte resistance. EDOT:SS TO 7 impedance'' / Ω Model Fit of the mpedance Spectra Series. +.V - +.7V ACN-TBA F +.7V - T - (oxidized) - EDOT:SS TO impedance' / Ω Modeling & fit of the oxidized states (left) and the model used (right).,: (slightly oxidized) hole transport layer with, porous distribution.,: (almost) fully oxidized active layer. : electrolyte resistance. ES, MS & MVS Joint Model Fit of the Reduced State. modulus phase / o K impedance / Ω m voltage eff. / V m - µ ACN-TBA F T 7 EDOT:SS TO Set-p for Dynamic Transmission / Reflection Measurements µ current eff. / A m - n m m K m m K TRFT-Modeling (solid lines) of the data (symbols) and the model used (inlay right).,: inert hole transport layer with, porous distribution.,: active layer redox Faraday impedance, film assigned diffusion, 7 layer capacity, photocurrent source with, porous distribution. 7 : electrolyte resistance. Setup consisting of a selective Light Source with supply potentiostat, the sample cell controlled by an additional slave potentiostat and the transmitted light sensor controlled by the Zennium main potententiostat Experimental Spectra ˆ + TR TR TR ˆ pot = = =, V ˆ e ˆ [ ] = pot ˆ + TR TR e TR ˆ gal = = = e, A ˆ e ˆ [ gal ] = pot gal c cˆ const = = ˆ e + c cˆ const = = ˆ + cˆ = e ˆ cˆ = e ˆ spectra of a the multilayer polymer film electrode TO - EDOT:SS - T in Acetonitrile / TBA-F at different wave lengths of nm (red curves) and 7 nm (blue curves)
e - Galvanic Cell 1. Voltage Sources 1.1 Polymer Electrolyte Membrane (PEM) Fuel Cell
Galvanic cells convert different forms of energy (chemical fuel, sunlight, mechanical pressure, etc.) into electrical energy and heat. In this lecture, we are interested in some examples of galvanic cells.
More informationChapter 3 Modeling and Simulation of Dye-Sensitized Solar Cell
Chapter 3 Modeling and Simulation of Dye-Sensitized Solar Cell 3.1. Introduction In recent years, dye-sensitized solar cells (DSSCs) based on nanocrystalline mesoporous TiO 2 films have attracted much
More informationSolar cells operation
Solar cells operation photovoltaic effect light and dark V characteristics effect of intensity effect of temperature efficiency efficency losses reflection recombination carrier collection and quantum
More informationOrganic Electronic Devices
Organic Electronic Devices Week 4: Organic Photovoltaic Devices Lecture 4.1: Overview of Organic Photovoltaic Devices Bryan W. Boudouris Chemical Engineering Purdue University 1 Lecture Overview and Learning
More informationPlanar Organic Photovoltaic Device. Saiful I. Khondaker
Planar Organic Photovoltaic Device Saiful I. Khondaker Nanoscience Technology Center and Department of Physics University of Central Florida http://www.physics.ucf.edu/~khondaker W Metal 1 L ch Metal 2
More informationREFRACTORY METAL OXIDES: FABRICATION OF NANOSTRUCTURES, PROPERTIES AND APPLICATIONS
REFRACTORY METAL OXIDES: FABRICATION OF NANOSTRUCTURES, PROPERTIES AND APPLICATIONS S.K. Lazarouk, D.A. Sasinovich BELARUSIAN STATE UNIVERSITY OF INFORMATICS AND RADIOELECTRONICS Outline: -- experimental
More informationChapter 22. Bulk Electrolysis: Electrogravimetry and Coulometry. Definition. Features of Bulk Electrolysis Cells
Chapter 22 Bulk Electrolysis: Electrogravimetry and Coulometry Definition Bulk Electrolysis deals with methods that involve electrolysis producing a quantitative change in oxidation state Example: In a
More informationNumerical simula,on of the performance of the dye sensi,zed solar cell
I Taller de Innovación Fotovoltaica y Celdas Solares; March 8 10, 2011, CIE UNAM, Temixco. Numerical simula,on of the performance of the dye sensi,zed solar cell Julio Villanueva Cab 1,*, Elena Guillén
More informationDemystifying Transmission Lines: What are They? Why are They Useful?
Demystifying Transmission Lines: What are They? Why are They Useful? Purpose of This Note This application note discusses theory and practice of transmission lines. It outlines the necessity of transmission
More informationand Technology, Luoyu Road 1037, Wuhan, , P. R. China. *Corresponding author. ciac - Shanghai P. R.
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry Supplementary Information For Journal of Materials Chemistry A Perovskite- @BiVO
More informationSolar Cell Materials and Device Characterization
Solar Cell Materials and Device Characterization April 3, 2012 The University of Toledo, Department of Physics and Astronomy SSARE, PVIC Principles and Varieties of Solar Energy (PHYS 4400) and Fundamentals
More informationAppendix 1: List of symbols
Appendix 1: List of symbols Symbol Description MKS Units a Acceleration m/s 2 a 0 Bohr radius m A Area m 2 A* Richardson constant m/s A C Collector area m 2 A E Emitter area m 2 b Bimolecular recombination
More informationElectrons are shared in covalent bonds between atoms of Si. A bound electron has the lowest energy state.
Photovoltaics Basic Steps the generation of light-generated carriers; the collection of the light-generated carriers to generate a current; the generation of a large voltage across the solar cell; and
More informationA. OTHER JUNCTIONS B. SEMICONDUCTOR HETEROJUNCTIONS -- MOLECULES AT INTERFACES: ORGANIC PHOTOVOLTAIC BULK HETEROJUNCTION DYE-SENSITIZED SOLAR CELL
A. OTHER JUNCTIONS B. SEMICONDUCTOR HETEROJUNCTIONS -- MOLECULES AT INTERFACES: ORGANIC PHOTOVOLTAIC BULK HETEROJUNCTION DYE-SENSITIZED SOLAR CELL February 9 and 14, 2012 The University of Toledo, Department
More informationSupporting Information. Fully Solution-Processed Semitransparent Organic Solar Cells with a Silver Nanowire Cathode and a Conducting Polymer Anode
Supporting Information Fully Solution-Processed Semitransparent Organic Solar Cells with a Silver Nanowire Cathode and a Conducting Polymer Anode Jong Hyuk Yim, Sung-yoon Joe, Christina Pang, Kyung Moon
More informationElectrochemistry of Semiconductors
Electrochemistry of Semiconductors Adrian W. Bott, Ph.D. Bioanalytical Systems, Inc. 2701 Kent Avenue West Lafayette, IN 47906-1382 This article is an introduction to the electrochemical properties of
More informationQ. Shen 1,2) and T. Toyoda 1,2)
Photosensitization of nanostructured TiO 2 electrodes with CdSe quntum dots: effects of microstructure in substrates Q. Shen 1,2) and T. Toyoda 1,2) Department of Applied Physics and Chemistry 1), and
More informationSupplementary Figure 3. Transmission spectrum of Glass/ITO substrate.
Supplementary Figure 1. The AFM height and SKPM images of PET/Ag-mesh/PH1000 and PET/Ag-mesh/PH1000/PEDOT:PSS substrates. (a, e) AFM height images on the flat PET area. (c, g) AFM height images on Ag-mesh
More informationSupplementary Figures
Supplementary Figures Supplementary Figure 1. AFM profiles of the charge transport and perovskite layers. AFM Image showing the thickness (y axis) of the layer with respect to the horizontal position of
More informationThe driving force dependence of charge Carrier dynamics in donor-acceptor Organic photovoltaic systems using Optical and electronic techniques
University of Wollongong Research Online University of Wollongong Thesis Collection 2017+ University of Wollongong Thesis Collections 2017 The driving force dependence of charge Carrier dynamics in donor-acceptor
More informationSupplementary Information
Supplementary Information Supplementary Figures Supplementary Figure S1. Change in open circuit potential ( OCP) of 1% W-doped BiVO 4 photoanode upon illumination with different light intensities. Above
More informationChapter 7. Solar Cell
Chapter 7 Solar Cell 7.0 Introduction Solar cells are useful for both space and terrestrial application. Solar cells furnish the long duration power supply for satellites. It converts sunlight directly
More informationSUPPLEMENTARY INFORMATION
doi:10.1038/nature17653 Supplementary Methods Electronic transport mechanism in H-SNO In pristine RNO, pronounced electron-phonon interaction results in polaron formation that dominates the electronic
More informationPhotovoltaics. Lecture 7 Organic Thin Film Solar Cells Photonics - Spring 2017 dr inż. Aleksander Urbaniak
Photovoltaics Lecture 7 Organic Thin Film Solar Cells Photonics - Spring 2017 dr inż. Aleksander Urbaniak Barcelona, Spain Perpignan train station, France source: pinterest Why organic solar cells? 1.
More informationCare of Computer-Controlled Potentiostats
Care of Computer-Controlled Potentiostats What is a Potentiostat? Potentiostat An electronic instrument that measures and controls the voltage difference between a Working Electrode and a Reference Electrode.
More informationNovel Devices and Circuits for Computing
Novel Devices and Circuits for Computing UCSB 594BB Winter 2013 Lecture 3: ECM cell Class Outline ECM General features Forming and SET process RESET Variants and scaling prospects Equivalent model Electrochemical
More informationSupporting Information
Supporting Information Red-absorbing Cationic Acceptor Dyes for Photocathodes in Tandem Solar Cells. Christopher J. Wood, a Ming Cheng, b Charlotte A. Clark, a Raphael Horvath, a Ian P. Clark, c Michelle
More informationSupplementary Figure S1. The maximum possible short circuit current (J sc ) from a solar cell versus the absorber band-gap calculated assuming 100%
Supplementary Figure S1. The maximum possible short circuit current (J sc ) from a solar cell versus the absorber band-gap calculated assuming 100% (black) and 80% (red) external quantum efficiency (EQE)
More informationMaria Carmela Di Piazza. Gianpaolo Vitale. Photovoltaic Sources. Modeling and Emulation. ^ Springer
Maria Carmela Di Piazza Gianpaolo Vitale Photovoltaic Sources Modeling and Emulation ^ Springer Part I 1 From the Nuclear Fusion to the Radiated Energy on the Earth... 3 1.1 Inside the Universe 3 1.2 The
More informationTheory of Electrical Characterization of Semiconductors
Theory of Electrical Characterization of Semiconductors P. Stallinga Universidade do Algarve U.C.E.H. A.D.E.E.C. OptoElectronics SELOA Summer School May 2000, Bologna (It) Overview Devices: bulk Schottky
More informationEnhanced Charge Extraction in Organic Solar Cells through. Electron Accumulation Effects Induced by Metal
Electronic Supplementary Information Enhanced Charge Extraction in Organic Solar Cells through Electron Accumulation Effects Induced by Metal Nanoparticles Feng-xian Xie, a Wallace C. H. Choy, * a Wei
More informationPHOTOVOLTAICS Fundamentals
PHOTOVOLTAICS Fundamentals PV FUNDAMENTALS Semiconductor basics pn junction Solar cell operation Design of silicon solar cell SEMICONDUCTOR BASICS Allowed energy bands Valence and conduction band Fermi
More informationIntroduction. Katarzyna Skorupska. Silicon will be used as the model material however presented knowledge applies to other semiconducting materials
Introduction Katarzyna Skorupska Silicon will be used as the model material however presented knowledge applies to other semiconducting materials 2 June 26 Intrinsic and Doped Semiconductors 3 July 3 Optical
More informationVI. EIS STUDIES LEAD NANOPOWDER
VI. EIS STUDIES LEAD NANOPOWDER 74 26. EIS Studies of Pb nanospheres Impedance (valid for both DC and AC), a complex resistance occurs when current flows through a circuit (composed of various resistors,
More informationElectrochemistry. Michael Faraday s law of electromagnetic induction says that whenever a conductor is
Surname 1 Name Course Instructor Date Electrochemistry 1. Faraday s Law Michael Faraday s law of electromagnetic induction says that whenever a conductor is positioned in a changeable magnetic field emf
More informationLab #5 Current/Voltage Curves, Efficiency Measurements and Quantum Efficiency
Lab #5 Current/Voltage Curves, Efficiency Measurements and Quantum Efficiency R.J. Ellingson and M.J. Heben November 4, 2014 PHYS 4580, 6280, and 7280 Simple solar cell structure The Diode Equation Ideal
More informationElectrochemical Cell - Basics
Electrochemical Cell - Basics The electrochemical cell e - (a) Load (b) Load e - M + M + Negative electrode Positive electrode Negative electrode Positive electrode Cathode Anode Anode Cathode Anode Anode
More informationVTS Process Photodiodes
VTS PROCESS LOW CAPACITANCE, LARGE AREA PHOTODIODE FEATURES Visible to IR spectral range Excellent QE - 400 to 1100 nm Guaranteed 400 nm response Response @ 940 nm, 0.60 A/W, typical Useable with visible
More informationA. OTHER JUNCTIONS B. SEMICONDUCTOR HETEROJUNCTIONS -- MOLECULES AT INTERFACES: ORGANIC PHOTOVOLTAIC BULK HETEROJUNCTION DYE-SENSITIZED SOLAR CELL
A. OTHER JUNCTIONS B. SEMICONDUCTOR HETEROJUNCTIONS -- MOLECULES AT INTERFACES: ORGANIC PHOTOVOLTAIC BULK HETEROJUNCTION DYE-SENSITIZED SOLAR CELL March 20, 2014 The University of Toledo, Department of
More informationOPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626
OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Announcements Homework #6 is assigned, due May 1 st Final exam May 8, 10:30-12:30pm
More informationLecture Note #13. Bard, ch. 18. Photoelectrochemistry (ch. 18) 1. Electrogenerated Chemiluminescence 2. Photoelectrochemistry at Semiconductors
Lecture Note #13 Photoelectrochemistry (ch. 18) 1. Electrogenerated Chemiluminescence 2. Photoelectrochemistry at Semiconductors Bard, ch. 18 Photoelectrochemistry Radiation energy electrical or chemical
More informationSupplementary material: Nature Nanotechnology NNANO D
Supplementary material: Nature Nanotechnology NNANO-06070281D Coercivities of the Co and Ni layers in the nanowire spin valves In the tri-layered structures used in this work, it is unfortunately not possible
More informationFlexible Organic Photovoltaics Employ laser produced metal nanoparticles into the absorption layer 1. An Introduction
Flexible Organic Photovoltaics Employ laser produced metal nanoparticles into the absorption layer 1. An Introduction Among the renewable energy sources that are called to satisfy the continuously increased
More informationPH575 Spring Lecture #20 Semiconductors: optical properties: Kittel Ch. 8 pp ; Ch 15 pp
PH575 Spring 2014 Lecture #20 Semiconductors: optical properties: Kittel Ch. 8 pp. 187-191; Ch 15 pp. 435-444 Figure VI-1-1: Different types of optical absorption phenomena; (1) transitions of highlying
More informationQualitative Picture of the Ideal Diode. G.R. Tynan UC San Diego MAE 119 Lecture Notes
Qualitative Picture of the Ideal Diode G.R. Tynan UC San Diego MAE 119 Lecture Notes Band Theory of Solids: From Single Attoms to Solid Crystals Isolated Li atom (conducting metal) Has well-defined, isolated
More informationA new concept of charging supercapacitors based on a photovoltaic effect
Electronic Supplementary Material (ESI) for ChemComm. This journal is The Royal Society of Chemistry 2016 Electronic supporting information (ESI) A new concept of charging supercapacitors based on a photovoltaic
More informationHigh-resolution on-chip supercapacitors with ultra-high scan rate ability
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry 214 Supporting Information High-resolution on-chip supercapacitors with ultra-high
More informationSpiro-Configured Bifluorenes: Highly Efficient Emitter for UV Organic Light-Emitting Device and Host Material for Red Electrophosphorescence
Spiro-Configured Bifluorenes: Highly Efficient Emitter for UV Organic Light-Emitting Device and Host Material for Red Electrophosphorescence Ken-Tsung Wong,* a Yuan-Li Liao, a Yu-Ting Lin, b Hai-Ching
More informationChapter 7. Conclusion and Future Scope
Chapter 7 Conclusion and Future Scope This chapter presents a summary of the work with concluding remarks for the research performed and reported in this thesis and then lays out the future scope pertaining
More informationA. OTHER JUNCTIONS B. SEMICONDUCTOR HETEROJUNCTIONS -- MOLECULES AT INTERFACES: ORGANIC PHOTOVOLTAIC BULK HETEROJUNCTION DYE-SENSITIZED SOLAR CELL
A. OTHER JUNCTIONS B. SEMICONDUCTOR HETEROJUNCTIONS -- MOLECULES AT INTERFACES: ORGANIC PHOTOVOLTAIC BULK HETEROJUNCTION DYE-SENSITIZED SOLAR CELL March 24, 2015 The University of Toledo, Department of
More informationMesoporous titanium dioxide electrolyte bulk heterojunction
Mesoporous titanium dioxide electrolyte bulk heterojunction The term "bulk heterojunction" is used to describe a heterojunction composed of two different materials acting as electron- and a hole- transporters,
More informationThe photovoltaic effect occurs in semiconductors where there are distinct valence and
How a Photovoltaic Cell Works The photovoltaic effect occurs in semiconductors where there are distinct valence and conduction bands. (There are energies at which electrons can not exist within the solid)
More informationPHYSICS nd TERM Outline Notes (continued)
PHYSICS 2800 2 nd TERM Outline Notes (continued) Section 6. Optical Properties (see also textbook, chapter 15) This section will be concerned with how electromagnetic radiation (visible light, in particular)
More informationFundamentals of Photovoltaics: C1 Problems. R.Treharne, K. Durose, J. Major, T. Veal, V.
Fundamentals of Photovoltaics: C1 Problems R.Treharne, K. Durose, J. Major, T. Veal, V. Dhanak @cdtpv November 3, 2015 These problems will be highly relevant to the exam that you will sit very shortly.
More informationSupplementary Figure 1. Supplementary Figure 1 Characterization of another locally gated PN junction based on boron
Supplementary Figure 1 Supplementary Figure 1 Characterization of another locally gated PN junction based on boron nitride and few-layer black phosphorus (device S1). (a) Optical micrograph of device S1.
More informationSupporting Information
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry 2018 Supporting Information A minimal non-radiative recombination loss for efficient
More informationPaper Review. Special Topics in Optical Engineering II (15/1) Minkyu Kim. IEEE Journal of Quantum Electronics, Feb 1985
Paper Review IEEE Journal of Quantum Electronics, Feb 1985 Contents Semiconductor laser review High speed semiconductor laser Parasitic elements limitations Intermodulation products Intensity noise Large
More informationCharacterization of electric charge carrier transport in organic semiconductors by time-of-flight technique
Characterization of electric charge carrier transport in organic semiconductors by time-of-flight technique Raveendra Babu Penumala Mentor: Prof. dr. Gvido Bratina Laboratory of Organic Matter Physics
More informationSupplementary Figure S1. Verifying the CH 3 NH 3 PbI 3-x Cl x sensitized TiO 2 coating UV-vis spectrum of the solution obtained by dissolving the
Supplementary Figure S1. Verifying the CH 3 NH 3 PbI 3-x Cl x sensitized TiO 2 coating UV-vis spectrum of the solution obtained by dissolving the spiro-ometad from a perovskite-filled mesoporous TiO 2
More informationPhotovoltaic cell and module physics and technology. Vitezslav Benda, Prof Czech Technical University in Prague
Photovoltaic cell and module physics and technology Vitezslav Benda, Prof Czech Technical University in Prague benda@fel.cvut.cz www.fel.cvut.cz 1 Outlines Photovoltaic Effect Photovoltaic cell structure
More informationEE 5344 Introduction to MEMS CHAPTER 5 Radiation Sensors
EE 5344 Introduction to MEMS CHAPTER 5 Radiation Sensors 5. Radiation Microsensors Radiation µ-sensors convert incident radiant signals into standard electrical out put signals. Radiant Signals Classification
More informationmaximal photofluorescence decay time of 6 hours (purchased from Shenzhen HuiDuoSheng
Electronic Supplementary Material (ESI) for ChemComm. This journal is The Royal Society of Chemistry 2017 Experimental section Preparation of m-tio 2 /LPP photoanodes. TiO 2 colloid was synthesized according
More informationEE 5611 Introduction to Microelectronic Technologies Fall Tuesday, September 23, 2014 Lecture 07
EE 5611 Introduction to Microelectronic Technologies Fall 2014 Tuesday, September 23, 2014 Lecture 07 1 Introduction to Solar Cells Topics to be covered: Solar cells and sun light Review on semiconductor
More informationTeaching the concept of energy using analogies between solar energy converters
Teaching the concept of using analogies between solar converters TPI-15 / ELTE Zoltán Csernovszky Kölcsey Ferenc High School, Budapest Physics Teaching PhD School, Eötvös University LIGHT Interactions
More informationContents. I Background 1. Contents... Preface... Acknowledgments... The Blind Men and the Elephant... xxi. History of Impedance Spectroscopy...
Contents Contents...................................... Preface....................................... Acknowledgments................................. v xv xix The Blind Men and the Elephant.......................
More informationCarbonized Electrospun Nanofiber Sheets for Thermophones
Supporting Information Carbonized Electrospun Nanofiber Sheets for Thermophones Ali E. Aliev 1 *, Sahila Perananthan 2, John P. Ferraris 1,2 1 A. G. MacDiarmid NanoTech Institute, University of Texas at
More information3/24/11. Introduction! Electrogenic cell
March 2011 Introduction Electrogenic cell Electrode/electrolyte interface Electrical double layer Half-cell potential Polarization Electrode equivalent circuits Biopotential electrodes Body surface electrodes
More informationSupplementary material for High responsivity mid-infrared graphene detectors with antenna-enhanced photo-carrier generation and collection
Supplementary material for High responsivity mid-infrared graphene detectors with antenna-enhanced photo-carrier generation and collection Yu Yao 1, Raji Shankar 1, Patrick Rauter 1, Yi Song 2, Jing Kong
More informationMaterials and Structural Design for Advanced Energy Storage Devices
Materials and Structural Design for Advanced Energy Storage Devices Imran Shakir Sustainable Energy Technologies Center (SET) King Saud University Saudi Arabia Specific Power (W/kg) Introduction and Motivation
More informationThermionic Current Modeling and Equivalent Circuit of a III-V MQW P-I-N Photovoltaic Heterostructure
Thermionic Current Modeling and Equivalent Circuit of a III-V MQW P-I-N Photovoltaic Heterostructure ARGYRIOS C. VARONIDES Physics and Electrical Engineering Department University of Scranton 800 Linden
More informationFYS 3028/8028 Solar Energy and Energy Storage. Calculator with empty memory Language dictionaries
Faculty of Science and Technology Exam in: FYS 3028/8028 Solar Energy and Energy Storage Date: 11.05.2016 Time: 9-13 Place: Åsgårdvegen 9 Approved aids: Type of sheets (sqares/lines): Number of pages incl.
More informationDeliverable D1.3 Demonstration of patterning processes allowing to
D.3 H2020-LCE-205- CHEOPS Production technology to achieve low Cost and Highly Efficient photovoltaic Perovskite Solar cells Deliverable D.3 WP Perovskite single junction development Authors: Soo-Jin Moon
More informationElectronic Supplementary Information: Synthesis and Characterization of Photoelectrochemical and Photovoltaic Cu2BaSnS4 Thin Films and Solar Cells
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry C. This journal is The Royal Society of Chemistry 2017 Electronic Supplementary Information: Synthesis and Characterization of
More informationA Fixed Surface Potential Probe with the Swing Capacitive Electrometer Compared to the Vibrating Kelvin Probe
Proc. 2017 Annual Meeting of the Electrostatics of America 1 A Fixed Surface Potential Probe with the Swing Capacitive Electrometer Compared to the Vibrating Kelvin Probe Michael Reznikov Dept. of Integrated
More informationPhotovoltaic Energy Conversion. Frank Zimmermann
Photovoltaic Energy Conversion Frank Zimmermann Solar Electricity Generation Consumes no fuel No pollution No greenhouse gases No moving parts, little or no maintenance Sunlight is plentiful & inexhaustible
More informationSolar Fuels From Light & Heat
Solar Fuels From Light & Heat Xiaofei Ye, Liming Zhang, Madhur Boloor, Nick Melosh Will Chueh Materials Science & Engineering, Precourt Institute for Energy Stanford University Sunita Williams, NASA 2
More informationBasic Limitations to Third generation PV performance
Basic Limitations to Third generation PV performance Pabitra K. Nayak Weizmann Institute of Science, Rehovot, Israel THANKS to my COLLEAGUES Lee Barnea and David Cahen. Weizmann Institute of Science Juan
More informationPotential Modulated Spectroscopy in Electrochemical Systems
Potential Modulated Spectroscopy in Electrochemical Systems David J. Fermín Action D36 www.chm.bris.ac.uk/pt/electrochemistry Overview Combining potential modulation and spectroscopy? Electroreflectance
More informationHole Selective NiO Contact for Efficient Perovskite Solar Cells with Carbon Electrode
Supporting information For Nano Letters Hole Selective NiO Contact for Efficient Perovskite Solar Cells with Carbon Electrode Xiaobao Xu,,, Zonghao Liu,, Zhixiang Zuo, Meng Zhang, Zhixin Zhao, Yan Shen,
More informationPhotoelectrochemical characterization of Bi 2 S 3 thin films deposited by modified chemical bath deposition
Indian Journal of Engineering & Materials Sciences Vol. 13, April; 2006, pp. 140-144 Photoelectrochemical characterization of Bi 2 S 3 thin films deposited by modified chemical bath deposition R R Ahire
More information17.1 Redox Chemistry Revisited
Chapter Outline 17.1 Redox Chemistry Revisited 17.2 Electrochemical Cells 17.3 Standard Potentials 17.4 Chemical Energy and Electrical Work 17.5 A Reference Point: The Standard Hydrogen Electrode 17.6
More informationConductivity and Semi-Conductors
Conductivity and Semi-Conductors J = current density = I/A E = Electric field intensity = V/l where l is the distance between two points Metals: Semiconductors: Many Polymers and Glasses 1 Electrical Conduction
More informationLecture 5 Junction characterisation
Lecture 5 Junction characterisation Jon Major October 2018 The PV research cycle Make cells Measure cells Despair Repeat 40 1.1% 4.9% Data Current density (ma/cm 2 ) 20 0-20 -1.0-0.5 0.0 0.5 1.0 Voltage
More informationFebruary 1, 2011 The University of Toledo, Department of Physics and Astronomy SSARE, PVIC
FUNDAMENTAL PROPERTIES OF SOLAR CELLS February 1, 2011 The University of Toledo, Department of Physics and Astronomy SSARE, PVIC Principles and Varieties of Solar Energy (PHYS 4400) and Fundamentals of
More information3.1 Absorption and Transparency
3.1 Absorption and Transparency 3.1.1 Optical Devices (definitions) 3.1.2 Photon and Semiconductor Interactions 3.1.3 Photon Intensity 3.1.4 Absorption 3.1 Absorption and Transparency Objective 1: Recall
More informationOrganic Electronic Devices
Organic Electronic Devices Week 4: Organic Photovoltaic Devices Lecture 4.2: Characterizing Device Parameters in OPVs Bryan W. Boudouris Chemical Engineering Purdue University 1 Lecture Overview and Learning
More informationBoron-doped graphene as high-efficiency counter electrode for dye-sensitized solar cells
Electronic Supplementary Information Boron-doped graphene as high-efficiency counter electrode for dye-sensitized solar cells Haiqiu Fang #, Chang Yu #, Tingli Ma, and Jieshan Qiu* Carbon Research Laboratory,
More informationCHAPTER-3 FABRICATION OF SOLID- LIQUID JUNCTION SOLAR CELL USING TMDCS CRYSTALS
CHAPTER-3 FABRICATION OF SOLID- LIQUID JUNCTION SOLAR CELL USING TMDCS CRYSTALS 72 3.1 INTRODUCTION: As the solid- liquid junction solar cells require only electron donating material and electron accepting
More informationInterdisciplinary Graduate School, Nanyang Technological University, Singapore , Singapore.
Electronic Supplementary Material (ESI) for Nanoscale. This journalelectronic is TheSupplementary Royal Society Information of Chemistry (ESI) for 2014 Nanoscale. Triple-layer nanostructured WO 3 photoanodes
More informationElectrodes MB - JASS 09. Metal in electrolyte
Electrodes MB - JASS 09 Metal in electrolyte 1 Helmholtz double layer (1) Helmholtz double layer : simplest approximation surface charge is neutralized by opposite signed counterions placed away from the
More informationChemistry Instrumental Analysis Lecture 18. Chem 4631
Chemistry 4631 Instrumental Analysis Lecture 18 Oxidation/Reduction Reactions Transfer of electrons in solution from one reactant to another. Ce +4 + Fe +2 Ce +3 + Fe +3 Ce +4 and Fe 3+ Fe 2+ and Ce 3+
More informationCHAPTER 6. ELECTROCHEMICAL OSCILLATIONS IN METHANOL OXIDATION
CHAPTER 6. ELECTROCHEMICAL OSCILLATIONS IN METHANOL OXIDATION 143 CHAPTER 6. ELECTROCHEMICAL OSCILLATIONS IN METHANOL OXIDATION 6.1 Introduction Based on the previous three experimental chapters dealing
More informationTowards a deeper understanding of polymer solar cells
Towards a deeper understanding of polymer solar cells Jan Anton Koster Valentin Mihailetchi Prof. Paul Blom Molecular Electronics Zernike Institute for Advanced Materials and DPI University of Groningen
More informationElectronic Supplementary Information. Recombination kinetics in silicon solar cell under low-concentration: Electroanalytical
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2014 Electronic Supplementary Information Recombination kinetics in silicon solar cell
More informationSemiconductor Optoelectronics Prof. M. R. Shenoy Department of Physics Indian Institute of Technology, Delhi
Semiconductor Optoelectronics Prof. M. R. Shenoy Department of Physics Indian Institute of Technology, Delhi Lecture - 1 Context and Scope of the Course (Refer Slide Time: 00:44) Welcome to this course
More informationBLUE PRINT FOR MODEL QUESTION PAPER 4
Unit Chapter Teaching Hours Marks allotted (VSA) mark (SA) 3 mark (SA) 5 mark (LA) 5 mark (NP) BLUE PRINT FOR MODEL QUESTION PAPER 4 SUBJECT : PHYSICS (33) CLASS : II PUC Topic Electric Charges and Fields
More informationELECTROCHEMICAL IMPEDANCE SPECTROSCOPY
ELECTROCHEMICAL IMPEDANCE SPECTROSCOPY MARK E. ORAZEM University of Florida BERNARD TRIBOLLET Universite Pierre et Marie Curie WILEY A JOHN WILEY & SONS, INC., PUBLICATION Contents Contents Preface Acknowledgments
More informationPhotovoltaic cell and module physics and technology
Photovoltaic cell and module physics and technology Vitezslav Benda, Prof Czech Technical University in Prague benda@fel.cvut.cz www.fel.cvut.cz 6/21/2012 1 Outlines Photovoltaic Effect Photovoltaic cell
More informationYixin Zhao and Kai Zhu*
Supporting Information CH 3 NH 3 Cl-Assisted One-Step Solution Growth of CH 3 NH 3 PbI 3 : Structure, Charge- Carrier Dynamics, and Photovoltaic Properties of Perovskite Solar Cells Yixin Zhao and Kai
More informationAvailable online at Energy Procedia 00 (2009) Energy Procedia 2 (2010) E-MRS Spring meeting 2009, Symposium B
Available online at www.sciencedirect.com Energy Procedia 00 (2009) 000 000 Energy Procedia 2 (2010) 169 176 Energy Procedia www.elsevier.com/locate/procedia www.elsevier.com/locate/procedia E-MRS Spring
More information