NUMERICAL SIMULATION and PERFORMANCE OPTIMIZATION of PEROVSKITE SOLAR CELL a THESIS in ELECTRICAL ENGINEERING Presented to the F
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Window Layer Structures for Chalcopyrite Thin-Film Solar Cells
Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 1951 Window Layer Structures for Chalcopyrite Thin-Film Solar Cells FREDRIK LARSSON ACTA UNIVERSITATIS UPSALIENSIS ISSN 1651-6214 ISBN 978-91-513-0984-2 UPPSALA urn:nbn:se:uu:diva-416751 2020 Dissertation presented at Uppsala University to be publicly examined in Häggsalen, Ångströmlaboratoriet, Lägerhyddsvägen 1, Uppsala, Friday, 18 September 2020 at 09:15 for the degree of Doctor of Philosophy. The examination will be conducted in English. Faculty examiner: Professor Daniel Lincot (French National Centre for Scientific Research (CNRS)). Abstract Larsson, F. 2020. Window Layer Structures for Chalcopyrite Thin-Film Solar Cells. Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 1951. 110 pp. Uppsala: Acta Universitatis Upsaliensis. ISBN 978-91-513-0984-2. This thesis aims to contribute to the development of improved window layer structures for chalcopyrite thin-film solar cells, with an emphasis on the buffer layer, to assist future reductions of the levelized cost of energy. This is realized by exploring the potential of existing materials and deposition processes, as well as developing new buffer layer processes based on atomic layer deposition (ALD). Ternary compound ALD processes are more complicated to control than when depositing binary compounds and the composition can be significantly different at the absorber interface as compared to the bulk. A method based on in-situ quartz crystal microbalance that can measure these compositional variations is demonstrated in the thesis. Furthermore, the addition of alkali- metal fluoride post-deposition treatments (PDTs) can further complicate ALD of buffer layers, due to residual salts that are formed on the absorber surface during a PDT process. -
Introduction to Perovskite Solar Cells in an Undergraduate Laboratory Exercise
Faculty of Health, Science and Technology Oscar Eklund Introduction to Perovskite Solar Cells in an Undergraduate Laboratory Exercise Bachelor’s Thesis, 15 ECTS Engineering Physics Date: 2019-06-04 Supervisor: Leif Ericsson Examiner: Thijs Jan Holleboom Karlstads Universitet 651 88 Karlstad Tfn 054-700 10 00 Fax 054-700 14 60 [email protected] www.kau.se Oscar Eklund Introduction Karlstad University Abstract The course Functional Materials at Karlstad University aims for undergraduates to study some of the functional materials of the 21st century. One of the hottest topics in photovoltaic research is hybrid organic-inorganic perovskite solar cells due to their easy methods of fabrication, cheap costs and potential for high power conversion efficiencies. A laboratory manual is compiled for the course, in which students are encouraged to build perovskite solar cells with a device architecture of FTO/TiO2/MAPbI3/CuSCN/Carbon/FTO using spin coating and annealing for testing in a solar simulator. The power conversion efficiency achieved with this method reaches 0.056 %, with suggestions for improvement when done by students. Absorption properties are examined using UV-vis spectroscopy and the band gap energy of MAPbI3 is established as 1.59 eV. By using these techniques, students will earn a greater understanding for one of the most relevant topics of photovoltaic research and different equipment used in its fabrication and characterization Sammanfattning Kursen Funktionella material på Karlstads universitet har som mål att studenter ska få studera några av 2000-talets funktionella material. Ett av de största ämnena inom solcellsforskning är hybrida organiska/icke-organiska perovskitsolceller eftersom de är lätta att tillverka, billiga och har potential för höga verkningsgrader. -
Generalized Detailed Balance Theory of Solar Cells
Generalized detailed balance theory of solar cells Von der Fakult¨at f¨ur Elektrotechnik und Informationstechnik der Rheinisch-Westf¨alischen Technischen Hochschule Aachen zur Erlangung des akademischen Grades eines Doktors der Ingenieurwissenschaften genehmigte Dissertation vorgelegt von Diplom-Ingenieur Thomas Kirchartz aus Karlsruhe Berichter: Universit¨atsprofessor Dr. rer. nat. habil. Uwe Rau Universit¨atsprofessor Dr. phil. Heinrich Kurz Tag der m¨undlichen Pr¨ufung: 6. Februar 2009 Diese Dissertation ist auf den Internetseiten der Hochschulbibliothek online verf¨ugbar. Contents Abstract 1 Zusammenfassung 5 1 Introduction 9 2 Fundamentals 13 2.1 The principle of detailed balance . 13 2.2 TheShockley-Queisserlimit . 14 2.3 Combining transport with detailed balance . 18 2.3.1 A two state solar cell model . 18 2.3.2 Theonesidedpn-junction . 21 2.3.3 Radiative limit for arbitrary mobilities . 23 2.4 Solar cell and light emitting diode . 24 2.5 Properties of optoelectronic devices - a brief summary . ....... 26 3 Detailed balance model for bipolar charge transport 31 3.1 Introduction................................ 31 3.2 pnandpintypesolarcells . 33 3.3 Superposition, ideality and reciprocity in pin-type solar cells . 37 3.4 Model ................................... 41 3.5 Application to quantum well solar cells . 43 3.5.1 Introduction............................ 43 3.5.2 Opticalresults........................... 45 3.5.3 Results for finite mobilities . 50 3.5.4 Results for non-radiative recombination . 54 i ii CONTENTS 3.5.5 Tandem solar cells . 58 3.5.6 Conclusions ............................ 60 4 Detailed balance model for excitonic and bipolar charge transport 63 4.1 Introduction................................ 63 4.2 Model ................................... 64 4.2.1 Excitonic and bipolar solar cells . -
Quantum Mechanics Electromotive Force
Quantum Mechanics_Electromotive force . Electromotive force, also called emf[1] (denoted and measured in volts), is the voltage developed by any source of electrical energy such as a batteryor dynamo.[2] The word "force" in this case is not used to mean mechanical force, measured in newtons, but a potential, or energy per unit of charge, measured involts. In electromagnetic induction, emf can be defined around a closed loop as the electromagnetic workthat would be transferred to a unit of charge if it travels once around that loop.[3] (While the charge travels around the loop, it can simultaneously lose the energy via resistance into thermal energy.) For a time-varying magnetic flux impinging a loop, theElectric potential scalar field is not defined due to circulating electric vector field, but nevertheless an emf does work that can be measured as a virtual electric potential around that loop.[4] In a two-terminal device (such as an electrochemical cell or electromagnetic generator), the emf can be measured as the open-circuit potential difference across the two terminals. The potential difference thus created drives current flow if an external circuit is attached to the source of emf. When current flows, however, the potential difference across the terminals is no longer equal to the emf, but will be smaller because of the voltage drop within the device due to its internal resistance. Devices that can provide emf includeelectrochemical cells, thermoelectric devices, solar cells and photodiodes, electrical generators,transformers, and even Van de Graaff generators.[4][5] In nature, emf is generated whenever magnetic field fluctuations occur through a surface. -
A Review Paper Ondevelopment in Material Used in Solar Pannel As
SSRG International Journal of Mechanical Engineering Volume 6 Issue 6, 35-41, June 2019 ISSN: 2348–8360 /doi: 10.14445/23488360/IJME-V6I6P107 © 2019 Seventh Sense Research Group® A Review Paper on Development in Material Used in Solar Pannel as Solar Cell Material Ankur Kumar Bansal, Dinesh Kumar, Dr. Mukesh Kumar M.tech Mechanical, AKTU Lucknow, India Abstract electron flow when photons from sunlight absorbed In the present era, While seeing the increasing and ejected electrons, leaving a hole that is further demand for energy and depletion of resources from filled by the surrounding electrons. This phenomenon which we obtained energy, solar energy suggest as is called the photovoltaic effect. The PV cell directs the best alternative energy resource. The light from the electrons in one direction, which gives rise to the the sun is not only a non-vanishing resource of flow of current. The amount of current is directly energy but also it is an Eco- Friendly resource of proportional to the humble of absorbed photons. So it energy(free from the environment pollution and can be easily said that PV cells are a variable current noise). It can easily compensate for the energy source. The first solar cell was built by Charles Fritts requirements fulfilled by the other resources, which in 1883 by the use of a thin layer of gold, and a are depleting and environment challenges, such as coating of selenium formed a junction. In the starting Fossil Fuel and petroleum deposits. era, the PCE was very low, about 1% only, but Basically, we receive solar energy from the further improvements make it increase. -
Solar Cells They Rely on Are Notoriously Expensive to Produce
THE PRESENT PROBLEM WITH SOLAR POWER is price. Ironically, sunlight, which is abundant beyond the energy needs of the entire human race and completely free, is frequently deemed too expensive to harness. Photovoltaic panels, systems to make them compatible with grid electricity, and batteries to squirrel away energy for when it’s cloudy—all these add cost. And while such hardware and installation costs will continue to diminish over time, the standard silicon solar cells they rely on are notoriously expensive to produce. Naturally, the scientific community has taken great interest in identifying alternative materials for solar cells. Solar-harvesting materials under development at Los Alamos and elsewhere include specialized thin films, organic layers, semi- conductor nanodevices, and others. Each has promise, and each has drawbacks. But a new class of challengers emerged a few years ago and has been improving with surprising speed since then. Known as perovskites, they are any crystalline material with the same broad class of chemical structure as a natural mineral of the same name. Perovskite solar cells are generally easy to work with, easy to adjust for improved performance, and very easy to afford. And in recent experi- mentation at Los Alamos, a particular recipe has been shown to reliably generate perovskite crystals that exhibit solar conversion efficiencies comparable to those of silicon. “Silicon solar cells are still the gold standard. They’re reliable and efficient, and they’ve been thoroughly demonstrated in the field,” says Los Alamos materials scientist Aditya Mohite. “I can’t wait to render them obsolete.” Anatomy of a cell A standard solar cell contains an active layer, usually silicon, sandwiched between two electrode layers. -
Summary of the High-Efficiency Crystalline Solar Cell Research Forum
SUMMARY OF THE HIGH-EFFICIENCY CRYSTALLINE SOLAR CELL RESEARCH FORUM UNIVERSITY OF PENNSYLVANIA M. Wolf Session I: OVERVIEW P. Landsberg Some Aspects of the Minority Carrier Lifetime in Silicon. C.T. Sah Review of Recombination Phenomena in Righ- Efficiency Solar Cells. Session 11: EGR EFFICIENCY CONCEPTS n. Wolf Silicon Solar Cell Efficiency Improvement: Status and Outlook. Some Practical Considerattons far Econoaical Back Contact Fovaaaticn on High-Efficiency Solar Cells. High-Efficiency Cell Concepts on Low-Cost Silicon Sheet. R, Swanson High Lifetime Silicon Processing. L. Olsen Silicon HINP Solar Cells. Session 111: SURFACE/INTERFACE EFFECTS D. Chadi Atomic Structure of the Annealed Si (111) Surface. L. Kazaerski Surface and Interface Characteristics, S. Lai Nitridation of SiO2 for Surface Passivatfon. S. Panash Surface Passivation and Junction Formation Using Low-Energy Hydrogen Implants. P, Grunthaner Chemical Structure of Interfaces. PLENARY SESS!ONS Session IV: BULK BPFRCTS E. Sirtl Structural Defects in Crystalline Silicon. C. Pierce Oxygen and Carbon Impurities and Related Defects in Silicon. T. Tan Current Understanding of Point Defects and Diffusion Processes in Silicon. G. Schwuttke Defects in Web Dendrite Silicon Ribbon Crystals and Their Influences on Hinority Carrier Lifetime. J. Hanoka EBLC Characterization and dydrogen Passivation in Silicon Sheet. A. Neugrsschel Measurement of Electrical Parameters and Current Components in the Bulk of Silicon Solar Cells. Session V: MODEL-- I NG - R. Schwartz Current Status of One and Two Dimensional Numer- ical Models: Successes and Limitations. M. Lamorte Application of Closed-Form Solution Using Re- cursion Relationship in Silicon Solar Cells. P. Lindholm PIenomena Simulation for Heavy Doping and Surface ! Recombination Velocity. -
Maria Jabeen Phd Thesis.Pdf
Design and Optimization of thin-film solar cell configuration structures using the Finite Element Method Dissertation submitted in partial fulfilment of the requirements for the degree of Doctor of Philosophy Author: Maria Jabeen Supervisor: Dr. Shyqyri Haxha Reader (FIET, FHEA, CEng, SMIEEE) Director of Graduates Head of Microwave Photonics and Sensors Department of Electronic Engineering School of Engineering, Physical and Mathematical Sciences Royal Holloway, University of London, Egham, Surrey, TW20 0EX, United Kingdom Royal Holloway University of London October 2020 Declaration of Authorship I ………Maria Jabeen……………. hereby declare that this thesis and the work presented in it is entirely my own. Where I have consulted the work of others, this is always clearly stated. I am aware of the University's regulations concerning plagiarism, including those regulations concerning disciplinary actions that may result from plagiarism. Any use of the works of any other author, in any form, is properly acknowledged at their point of use. This work is confidential and should not be shared with anyone without prior consent of the PhD Supervisor (Dr. Shyqyri Haxha). Signed: ____ __________________ Name (in capitals): _____MARIA JABEEN_____________ Date: ______02-10-2020__________________ Abstract To make solar energy more feasible, the solar cells efficiency must increase and its cost of production must decrease in order to generate on a large scale. Thin-film photovoltaic solar cells exhibit the prospects of increasing efficiency and decreasing material costs. Research in plasmonic nanoparticles structures, textured interfaces and branched nano wire solar cells is still relatively new compared to thin-film bulk silicon solar cells. Nanostructured materials are being investigated and developed as versatile components of optoelectronic devices with the ability to manipulate light (via plasmonic enhancement, photonic crystals, and so on) and control energy flow at nearly the atomic level. -
Hybrid Nanocomposite Thin Films for Photovoltaic Applications: a Review
nanomaterials Review Hybrid Nanocomposite Thin Films for Photovoltaic Applications: A Review Marcela Socol *,† and Nicoleta Preda *,† National Institute of Materials Physics, 405A Atomistilor Street, P.O. Box MG-7, 077125 Magurele, Romania * Correspondence: marcela.socol@infim.ro (M.S.); nicol@infim.ro (N.P.) † These authors contributed equally. Abstract: Continuing growth in global energy consumption and the growing concerns regarding climate change and environmental pollution are the strongest drivers of renewable energy deploy- ment. Solar energy is the most abundant and cleanest renewable energy source available. Nowadays, photovoltaic technologies can be regarded as viable pathways to provide sustainable energy genera- tion, the achievement attained in designing nanomaterials with tunable properties and the progress made in the production processes having a major impact in their development. Solar cells involving hybrid nanocomposite layers have, lately, received extensive research attention due to the possibility to combine the advantages derived from the properties of both components: flexibility and process- ability from the organic part and stability and optoelectronics features from the inorganic part. Thus, this review provides a synopsis on hybrid solar cells developed in the last decade which involve composite layers deposited by spin-coating, the most used deposition method, and matrix-assisted pulsed laser evaporation, a relatively new deposition technique. The overview is focused on the hybrid nanocomposite films that can use conducting polymers and metal phthalocyanines as p-type materials, fullerene derivatives and non-fullerene compounds as n-type materials, and semiconductor nanostructures based on metal oxide, chalcogenides, and silicon. A survey regarding the influence of various factors on the hybrid solar cell efficiency is given in order to identify new strategies for Citation: Socol, M.; Preda, N. -
Vince Thesis Online
KELVIN PROBE EXAMINATION OF ORGANIC/METALLIC SEMICONDUCTORS ______________________________________ A Thesis Presented to The Honors Tutorial College Ohio University ______________________________________ In Partial Fulfillment of the Requirements for Graduation from the Honors Tutorial College with the degree of Bachelor of Science in Physics ______________________________________ By Vincent Roberts June 2012 Table of Contents I. Introduction 4 A. An Energy Crisis 4 B. The Advent of the Solar Cell 6 II. Background and Theory 8 A. Solar Cell Technology: The Photoelectric . 8 B. Work Function and Charge Transfer . 11 C. Background on Kelvin Probe 15 D. “Seeing” at the Quantum Level 18 E. Principles of the Kelvin Method 19 III. Molecules and Preparation 25 A. Organic Molecule F4-TCNQ 25 B. Zinc Oxide 29 C. Sample Substrate Preparation 32 D. F4-TCNQ Preparation 34 IV. Data Collection 35 A. Kelvin Probe Preparation 35 B. Sample Probing 37 --2-- C. Data Collection Parameters 41 D. Discerning Between Good and Bad Data 42 V. Results and Conclusions 45 A. Discussion 45 B. Conclusions 50 C. Suggestion for Further Experimentation 54 Acknowledgements 56 References 57 --3-- I. Introduction An Energy Crisis Nano- and quantum technology are terms often used in science- fiction during the past several decades. They have become very much akin to “buzz” words of modern-day companies and technologies. The world is in the midst of a technological boom, yet it is also in a severe energy crisis. It’s no exaggeration to say that fossil fuels will be running short in the foreseeable future, and the call by environmentalists to save the planet have only added flames to the proverbial fire regarding the question of humanity’s sustainable energy dilemma. -
Advances in Cost-Efficient Thin-Film Photovoltaics Based on Cu(In,Ga)Se2
Engineering 3 (2017) 445–451 Contents lists available at ScienceDirect Engineering journal homepage: www.elsevier.com/locate/eng Research Clean Energy—Review Advances in Cost-Efficient Thin-Film Photovoltaics Based on Cu(In,Ga)Se2 Michael Powalla*, Stefan Paetel, Dimitrios Hariskos, Roland Wuerz, Friedrich Kessler, Peter Lechner, Wiltraud Wischmann, Theresa Magorian Friedlmeier Centre for Solar Energy and Hydrogen Research Baden-Württemberg (ZSW), Stuttgart 70563, Germany a r t i c l e i n f o a b s t r a c t Article history: In this article, we discuss the leading thin-film photovoltaic (PV) technology based on the Cu(In,Ga)Se2 (CIGS) Received 3 May 2017 compound semiconductor. This contribution includes a general comparison with the conventional Si-wafer- Revised 9 July 2017 based PV technology and discusses the basics of the CIGS technology as well as advances in world- Accepted 10 July 2017 record-level conversion efficiency, production, applications, stability, and future developments with respect Available online 11 August 2017 to a flexible product. Once in large-scale mass production, the CIGS technology has the highest potential of all PV technologies for cost-efficient clean energy generation. Keywords: © 2017 THE AUTHORS. Published by Elsevier LTD on behalf of the Chinese Academy of Engineering and Thin-film photovoltaics Higher Education Press Limited Company. This is an open access article under the CC BY-NC-ND Solar energy license (http://creativecommons.org/licenses/by-nc-nd/4.0/). Flexible Cu(In,Ga)Se2 1. Introduction 2. General comparison of CIGS-based thin-film and Si-wafer- based PV technologies Photovoltaic (PV) technology, which directly generates electricity from sunlight, is quickly becoming a major player in the future clean A solar cell is basically a large-area semiconductor diode. -
From the GKLS Equation to the Theory of Solar and Fuel Cells 1 Arxiv
From the GKLS equation to the theory of solar and fuel cells 1 R. Alicki Institute of Theoretical Physics and Astrophysics University of Gda´nsk,Poland Abstract The mathematically sound theory of quantum open systems, for- mulated in the 70-ties of XX century and highlighted by the discovery of Gorini-Kossakowski-Lindblad-Sudarshan (GKLS) equation, found a wide range of applications in various branches of physics and chem- istry, notably in the field of quantum information and quantum ther- modynamics. However, it took 40 years before this formalism has been applied to explain correctly the operation principles of long ex- isting energy transducers like photovoltaic, thermoelectric and fuel cells. This long path is briefly reviewed from the personal author's perspective. Finally, the new, fully quantum model of chemical en- gine based on GKLS equation and applicable to fuel cells or replica- tors is outlined. The model illustrates the difficulty with an entirely quantum operational definition of work, comparable to the Problem of Quantum Measurement. 1 Introduction In the miraculous year 1976 two independent papers by Lindblad [1] and Gorini{Kossakowski{Sudarshan [2] established the general form of the Markovian Master Equation for the density matrix ρ(t) of the open system satisfying complete positivity condition (~ ≡ 1) arXiv:1706.10257v1 [quant-ph] 30 Jun 2017 d 1 X ρ = −i[H; ρ] + ([V ρ, V y] + [V ; ρV y]) ≡ −i[H; ρ] + Lρ : (1) dt 2 j j j j j 1Based on the talk given at the 48 Symposium on Mathematical Physics : Gorini- Kossakowski-Lindblad-Sudarshan Master Equation - 40 Years After, Toru´n,June 10-12, 2016 1 The Hisenberg picture version of GKLS equation, valid for system's time- dependent operator X(t) d 1 X X = i[H; X] + (V y[X; V ] + [V y;X]V ) ≡ i[H; X] + L∗X (2) dt 2 j j j j j is also useful.