Quantitative Model of PV Cells The Illuminated Diode. G.R. Tynan UC San Diego MAE 119 Lecture Notes

Size: px
Start display at page:

Download "Quantitative Model of PV Cells The Illuminated Diode. G.R. Tynan UC San Diego MAE 119 Lecture Notes"

Transcription

1 Quantitativ Modl of PV Clls T Illuminatd Diod G.R. Tynan UC San Digo MAE 119 ctur Nots

2 WE FOUND WHAT WE SEEK: JJ(V) Currnt Dnsity vs Voltag Across Diod: J total qdn p qd pn J + J kt ( xp( qv / ) 1) Total Currnt, I (Amps), Is Just Jtotal * Ara of Diod ( xp( qv / ) 1) I( V ) I0 kt qdn p qd p 0 n0 I 0 A +

3 I-V Caractristics of p-n diod

4 Basics of Solar PV Clls Ky Concpts Poton Enrgy Spctrum Carg Carrir Gnration Via Poton Absorption Carg Carrir oss Mcanisms Un-illuminatd p-n junction diod Illuminatd p-n junction diod: T Solar PV Cll Solar PV Cll s as an Elctricity Sourc

5 Calculating Effct of Illumination wit E > Egap Potons Assum - gnration rat G constant Corrsponds to Epoton ~ Egap Flux Earlir Assumptions Still Valid Quasinutral Rgion, Dpltion Rgion Drift Currnt Dnsity ~ Diffusiv Dnsity in Dpltion Rgion Small minority carrir population Diffusiv minority carrir transport in quasinutral rgion

6 Poton absorption in smiconductor For Poton Enrgy, E n > E gap Poton Is Adsorbd & Crats /ol pair At Adsorption Sit:

7 Poton absorption in smiconductor For Poton Enrgy, E n < E gap Poton May b Adsorbd BUT DOES NOT CREATE /ol pair Or (mor likly) it passs troug matrial:

8 Approximat /ol Gnration Rat Assum All Potons Hav Enoug Enrgy to Crat /ol Pairs Tn G Is G ( 1 R) αn xp( xα) Poton Flux vs Distanc into PV Cll N(x) Numbr of Potons/Unit Ara/Unit Tim PV Cll x

9 Approximat /ol Gnration Rat For Wak Adsorption Approximat Gnration Rat, G (units: /ol pairs/unit volum/unit tim) G ~ ( 1 R) αn R fraction of ligt rflctd from surfac (R~0.05 wit Anti-rflction coating) N numbr potons/unit ara/unit tim a poton intnsity -folding attnuation lngt Typically fw microns

10 Typical Adsorption Cofficint Data for Ga-As Typical Pnntration Dpt for E>Egap,: 1/a~1 micron Data for Silicon Not Too Diffrnt

11 Basics of Solar PV Clls Ky Concpts Poton Enrgy Spctrum Carg Carrir Gnration Via Poton Absorption Carg Carrir oss Mcanisms Un-illuminatd p-n junction diod Illuminatd p-n junction diod: T Solar PV Cll Solar PV Cll s as an Elctricity Sourc

12 Effct of Illumination on diod MINORITY CHARGE CARRIER DISTRIBUTION: Diffusion Eqn for ol population distribution d dx Gnral Solution p n Δp 2 Δp 2 Gτ Δp + C G 2 D x + D x Us Sam Boundary Conditions to find Particular Solution qv kt pn + G + [ pn ( 1] ( x) τ 0 0 x Similar Rsult for Elctrons Holds

13 Effct of Illumination on diod MINORITY CHARGE CARRIER CURRENT: Currnt is Diffusiv, I.. J ~ dp/dx, J ~dn/dx è J J ( x) ( x') qd qd p n n p 0 0 ( ( qv kt qv kt 1) 1) x x' qg qg x x' Nxt, nd currnt across junction

14 Nd Currnt Flow in Dpltion Rgion (aka Transition Rgion or Junction) Currnt continuity quation givs 1 q dj dx ( U G) 1 q dj dx Nglct osss in Junction & Intgrat across junction to find cang in currnt: 0 W δj δj q Gdx ~ qgw (sinc G ~ constant)

15 Distribution of carrirs wit Illumination

16 Diod Rspons w/ Illumination: Currnt Dnsity vs Voltag Across Diod: J total qd n p J J qd dj p n 0 ( xp( qv / kt ) 1) + qgw Total Currnt, I (Amps), Is Just Jtotal * Ara of Diod I I I 0 ( qv kt qag( 1) I + W + )

17 Illuminatd p-n diod V mp Powr, PI V Voltag, V

18 Caractrizing Solar PV Cll Prformanc Opn Circuit Voltag, Voc Sort-circuit Currnt, Maximum Powr Point (Vmp,Imp) Fill Factor, V FF V MP OC V oc kt q I ln( I 0 + 1) I I qag( + W + ) I I SC MP SC Typically FF~ Efficincy η V I P MP in MP V I P OC in SC ~

19 Solar Poton Flux Spctrum & Maximum Sort-Circuit Currnt

20 Solar Cll Efficincy imits On Poton > On -ol pair + Trmal Enrgy Rcombination osss (Surfacs, Dfcts, Impuritis) Rflctions & Scattring

21 Basics of Solar PV Clls Ky Concpts Poton Enrgy Spctrum Carg Carrir Gnration Via Poton Absorption Carg Carrir oss Mcanisms Un-illuminatd p-n junction diod Illuminatd p-n junction diod: T Solar PV Cll Solar PV Cll s as an Elctricity Sourc

Quantitative Model of Unilluminated Diode part II. G.R. Tynan UC San Diego MAE 119 Lecture Notes

Quantitative Model of Unilluminated Diode part II. G.R. Tynan UC San Diego MAE 119 Lecture Notes Quantitativ Modl of Unilluminatd Diod part II G.R. Tynan UC San Digo MAE 119 Lctur Nots Minority Carrir Dnsity at dg of quasinutral rgion incrass EXPONENTIALLY forward bias p nb n pa = p n0 xp qv a kt

More information

EE 5611 Introduction to Microelectronic Technologies Fall Tuesday, September 23, 2014 Lecture 07

EE 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 information

Qualitative 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 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 information

Assignment # (1.0 %), 5.2 (0.6 %), 5.3 (1.0 %), 5.5 (0.4 %), 5.8 (1.0 %), 5.9 (0.4 %), 5.10 (0.6 %)

Assignment # (1.0 %), 5.2 (0.6 %), 5.3 (1.0 %), 5.5 (0.4 %), 5.8 (1.0 %), 5.9 (0.4 %), 5.10 (0.6 %) ELEC4/1-1 Assignmnt 4 1 Assignmnt #4..1 (1. %),. (.6 %),.3 (1. %),. (.4 %),.8 (1. %),.9 (.4 %),. (.6 %).1. Band gap and potodtction. a) a) Dtrmin t maximum valu of t nrgy gap (bandgap) wic a smiconductor,

More information

The pn junction: 2 Current vs Voltage (IV) characteristics

The pn junction: 2 Current vs Voltage (IV) characteristics Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n

More information

PHOTOVOLTAICS Fundamentals

PHOTOVOLTAICS 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 information

Solar cells operation

Solar 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 information

Lecture 18 - Semiconductors - continued

Lecture 18 - Semiconductors - continued Lctur 18 - Smiconductors - continud Lctur 18: Smiconductors - continud (Kittl C. 8) + a - Donors and accptors Outlin Mor on concntrations of lctrons and ols in Smiconductors Control of conductivity by

More information

Lecture #15. Bipolar Junction Transistors (BJTs)

Lecture #15. Bipolar Junction Transistors (BJTs) ctur #5 OUTN Th iolar Junction Transistor Fundamntals dal Transistor Analysis Rading: hatr 0,. 30 ctur 5, Slid iolar Junction Transistors (JTs Ovr th ast 3 ads, th highr layout dnsity and low-owr advantag

More information

Physics 43 HW #9 Chapter 40 Key

Physics 43 HW #9 Chapter 40 Key Pysics 43 HW #9 Captr 4 Ky Captr 4 1 Aftr many ours of dilignt rsarc, you obtain t following data on t potolctric ffct for a crtain matrial: Wavlngt of Ligt (nm) Stopping Potntial (V) 36 3 4 14 31 a) Plot

More information

3.003 Principles of Engineering Practice

3.003 Principles of Engineering Practice 3.003 Principles of Engineering Practice One Month Review Solar Cells The Sun Semiconductors pn junctions Electricity 1 Engineering Practice 1. Problem Definition 2. Constraints 3. Options 4. Analysis

More information

FYS 3028/8028 Solar Energy and Energy Storage. Calculator with empty memory Language dictionaries

FYS 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 information

Lecture 10 - Carrier Flow (cont.) February 28, 2007

Lecture 10 - Carrier Flow (cont.) February 28, 2007 6.720J/3.43J Integrated Microelectronic Devices - Spring 2007 Lecture 10-1 Lecture 10 - Carrier Flow (cont.) February 28, 2007 Contents: 1. Minority-carrier type situations Reading assignment: del Alamo,

More information

n N D n p = n i p N A

n N D n p = n i p N A Summary of electron and hole concentration in semiconductors Intrinsic semiconductor: E G n kt i = pi = N e 2 0 Donor-doped semiconductor: n N D where N D is the concentration of donor impurity Acceptor-doped

More information

Photovoltaic 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 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 information

Photovoltaic cell and module physics and technology

Photovoltaic 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 information

Solar Cell Physics: recombination and generation

Solar Cell Physics: recombination and generation NCN Summer School: July 2011 Solar Cell Physics: recombination and generation Prof. Mark Lundstrom lundstro@purdue.edu Electrical and Computer Engineering Purdue University West Lafayette, Indiana USA

More information

Lab #5 Current/Voltage Curves, Efficiency Measurements and Quantum Efficiency

Lab #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 information

Status of LAr TPC R&D (2) 2014/Dec./23 Neutrino frontier workshop 2014 Ryosuke Sasaki (Iwate U.)

Status of LAr TPC R&D (2) 2014/Dec./23 Neutrino frontier workshop 2014 Ryosuke Sasaki (Iwate U.) Status of LAr TPC R&D (2) 214/Dc./23 Nutrino frontir workshop 214 Ryosuk Sasaki (Iwat U.) Tabl of Contnts Dvlopmnt of gnrating lctric fild in LAr TPC Introduction - Gnrating strong lctric fild is on of

More information

Optoelectronics EE/OPE 451, OPT 444 Fall 2009 Section 1: T/Th 9:30 10:55 PM

Optoelectronics EE/OPE 451, OPT 444 Fall 2009 Section 1: T/Th 9:30 10:55 PM Optolctronics EE/OPE 451, OPT 444 Fall 009 Sction 1: T/Th 9:30 10:55 PM John D. Williams, Ph.D. Dpartmnt of Elctrical and Computr Enginring 406 Optics uilding UAHuntsvill, Huntsvill, AL 35899 Ph. (56)

More information

Ideal Diode Equation II + Intro to Solar Cells

Ideal Diode Equation II + Intro to Solar Cells ECE-35: Spring 15 Ideal Diode Equation II + Intro to Solar Cells Professor Mark Lundstrom Electrical and Computer Engineering Purdue University, West Lafayette, IN USA lundstro@purdue.edu Pierret, Semiconductor

More information

ECE-305: Spring 2018 Exam 2 Review

ECE-305: Spring 2018 Exam 2 Review ECE-305: Spring 018 Exam Review Pierret, Semiconductor Device Fundamentals (SDF) Chapter 3 (pp. 75-138) Chapter 5 (pp. 195-6) Professor Peter Bermel Electrical and Computer Engineering Purdue University,

More information

Lecture 15 - The pn Junction Diode (I) I-V Characteristics. November 1, 2005

Lecture 15 - The pn Junction Diode (I) I-V Characteristics. November 1, 2005 6.012 - Microelectronic Devices and Circuits - Fall 2005 Lecture 15-1 Lecture 15 - The pn Junction Diode (I) I-V Characteristics November 1, 2005 Contents: 1. pn junction under bias 2. I-V characteristics

More information

Characteristics of Gliding Arc Discharge Plasma

Characteristics of Gliding Arc Discharge Plasma Caractristics of Gliding Arc Discarg Plasma Lin Li( ), Wu Bin(, Yang Ci(, Wu Cngkang ( Institut of Mcanics, Cins Acadmy of Scincs, Bijing 8, Cina E-mail: linli@imc.ac.cn Abstract A gliding arc discarg

More information

ECE507 - Plasma Physics and Applications

ECE507 - Plasma Physics and Applications ECE507 - Plasma Physics and Applications Lctur 7 Prof. Jorg Rocca and Dr. Frnando Tomasl Dpartmnt of Elctrical and Computr Enginring Collisional and radiativ procsss All particls in a plasma intract with

More information

Last time. Resistors. Circuits. Question. Quick Quiz. Quick Quiz. ( V c. Which bulb is brighter? A. A B. B. C. Both the same

Last time. Resistors. Circuits. Question. Quick Quiz. Quick Quiz. ( V c. Which bulb is brighter? A. A B. B. C. Both the same Last tim Bgin circuits Rsistors Circuits Today Rsistor circuits Start rsistor-capacitor circuits Physical layout Schmatic layout Tu. Oct. 13, 2009 Physics 208 Lctur 12 1 Tu. Oct. 13, 2009 Physics 208 Lctur

More information

For the following statements, mark ( ) for true statement and (X) for wrong statement and correct it.

For the following statements, mark ( ) for true statement and (X) for wrong statement and correct it. Benha University Faculty of Engineering Shoubra Electrical Engineering Department First Year communications. Answer all the following questions Illustrate your answers with sketches when necessary. The

More information

Lecture 20 - p-n Junction (cont.) October 21, Non-ideal and second-order effects

Lecture 20 - p-n Junction (cont.) October 21, Non-ideal and second-order effects 6.70J/3.43J - Integrated Microelectronic Devices - Fall 00 Lecture 0-1 Lecture 0 - p-n Junction (cont.) October 1, 00 Contents: 1. Non-ideal and second-order effects Reading assignment: del Alamo, Ch.

More information

IVE(TY) Department of Engineering E&T2520 Electrical Machines 1 Miscellaneous Exercises

IVE(TY) Department of Engineering E&T2520 Electrical Machines 1 Miscellaneous Exercises TRANSFORMER Q1 IE(TY) Dpartmnt of Enginring E&T50 Elctrical Machins 1 Miscllanous Exrciss Q Q3 A singl phas, 5 ka, 0/440, 60 Hz transformr gav th following tst rsults. Opn circuit tst (440 sid opn): 0

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator. Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r

More information

High Energy Physics. Lecture 5 The Passage of Particles through Matter

High Energy Physics. Lecture 5 The Passage of Particles through Matter High Enrgy Physics Lctur 5 Th Passag of Particls through Mattr 1 Introduction In prvious lcturs w hav sn xampls of tracks lft by chargd particls in passing through mattr. Such tracks provid som of th most

More information

Chapter 7. Solar Cell

Chapter 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 information

Recitation 17: BJT-Basic Operation in FAR

Recitation 17: BJT-Basic Operation in FAR Recitation 17: BJT-Basic Operation in FAR BJT stands for Bipolar Junction Transistor 1. Can be thought of as two p-n junctions back to back, you can have pnp or npn. In analogy to MOSFET small current

More information

Carriers Concentration in Semiconductors - VI. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India

Carriers Concentration in Semiconductors - VI. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India Carrirs Conntration in Smionutors - VI 1 Prof.P. Ravinran, Dpartmnt of Pysis, Cntral Univrsity of Tamil au, Inia ttp://folk.uio.no/ravi/smi01 P.Ravinran, PHY0 Smionutor Pysis, 17 January 014 : Carrirs

More information

Getting J e (x), J h (x), E(x), and p'(x), knowing n'(x) Solving the diffusion equation for n'(x) (using p-type example)

Getting J e (x), J h (x), E(x), and p'(x), knowing n'(x) Solving the diffusion equation for n'(x) (using p-type example) 6.012 - Electronic Devices and Circuits Lecture 4 - Non-uniform Injection (Flow) Problems - Outline Announcements Handouts - 1. Lecture Outline and Summary; 2. Thermoelectrics Review Thermoelectricity:

More information

2. Background Material

2. Background Material S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds

More information

( )! N D ( x) ) and equilibrium

( )! N D ( x) ) and equilibrium ECE 66: SOLUTIONS: ECE 66 Homework Week 8 Mark Lundstrom March 7, 13 1) The doping profile for an n- type silicon wafer ( N D = 1 15 cm - 3 ) with a heavily doped thin layer at the surface (surface concentration,

More information

Comparison of Ge, InGaAs p-n junction solar cell

Comparison of Ge, InGaAs p-n junction solar cell ournal of Physics: Conference Series PAPER OPEN ACCESS Comparison of Ge, InGaAs p-n junction solar cell To cite this article: M. Korun and T. S. Navruz 16. Phys.: Conf. Ser. 77 135 View the article online

More information

February 1, 2011 The University of Toledo, Department of Physics and Astronomy SSARE, PVIC

February 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 information

Homework 6 Solar PV Energy MAE 119 W2017 Professor G.R. Tynan

Homework 6 Solar PV Energy MAE 119 W2017 Professor G.R. Tynan Homework 6 Solar PV Energy MAE 119 W2017 Professor G.R. Tynan 1. What is the most likely wavelength and frequency of light emitted from the sun which has a black body temperature of about 6600 deg K? What

More information

Lecture 16 - The pn Junction Diode (II) Equivalent Circuit Model. April 8, 2003

Lecture 16 - The pn Junction Diode (II) Equivalent Circuit Model. April 8, 2003 6.012 - Microelectronic Devices and Circuits - Spring 2003 Lecture 16-1 Lecture 16 - The pn Junction Diode (II) Equivalent Circuit Model April 8, 2003 Contents: 1. I-V characteristics (cont.) 2. Small-signal

More information

Pair (and Triplet) Production Effect:

Pair (and Triplet) Production Effect: Pair (and riplt Production Effct: In both Pair and riplt production, a positron (anti-lctron and an lctron (or ngatron ar producd spontanously as a photon intracts with a strong lctric fild from ithr a

More information

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017 Th following qustions ar to b answrd individually. Usful information such as tabls with dtctor charactristics and graphs with th proprtis of matrials ar availabl in th cours wb sit: http://www.lip.pt/~patricia/fisicadaradiacao.

More information

Carriers Concentration and Current in Semiconductors

Carriers Concentration and Current in Semiconductors Carriers Concentration and Current in Semiconductors Carrier Transport Two driving forces for carrier transport: electric field and spatial variation of the carrier concentration. Both driving forces lead

More information

Quiz #1 Due 9:30am Session #10. Quiz Instructions

Quiz #1 Due 9:30am Session #10. Quiz Instructions 2.626/2.627 Fall 2011 Fundamentals of Photovoltaics Quiz #1 Due 9:30am Session #10 Quiz Instructions The undergraduate version of this quiz (2.627) consists of four (4) multipart questions for a point

More information

Module 8 Non equilibrium Thermodynamics

Module 8 Non equilibrium Thermodynamics Modul 8 Non quilibrium hrmodynamics ctur 8.1 Basic Postulats NON-EQUIIRIBIUM HERMODYNAMICS Stady Stat procsss. (Stationary) Concpt of ocal thrmodynamic qlbm Extnsiv proprty Hat conducting bar dfin proprtis

More information

A. K. Das Department of Physics, P. K. College, Contai; Contai , India.

A. K. Das Department of Physics, P. K. College, Contai; Contai , India. IOSR Journal of Applied Physics (IOSR-JAP) e-issn: 2278-4861.Volume 7, Issue 2 Ver. II (Mar. - Apr. 2015), PP 08-15 www.iosrjournals.org Efficiency Improvement of p-i-n Structure over p-n Structure and

More information

Supplementary Information of. The Role of Fullerenes in Environmental Stability of Polymer:Fullerene Solar Cells

Supplementary Information of. The Role of Fullerenes in Environmental Stability of Polymer:Fullerene Solar Cells Electronic Supplementary Material (ESI) for Energy & Environmental Science. This journal is The Royal Society of Chemistry 2018 Supplementary Information of The Role of Fullerenes in Environmental Stability

More information

From Classical to Quantum mechanics

From Classical to Quantum mechanics From Classical to Quantum mcanics Engl & Rid 99-300 vrij Univrsitit amstrdam Classical wav baviour Ligt is a wav Two-slit xprimnt wit potons (81-85) 1 On sourc Intrfrnc sourcs ttp://www.falstad.com/matpysics.tml

More information

Simulations des micro-décharges de type MHCD

Simulations des micro-décharges de type MHCD Simulations ds micro-déchargs d typ MHCD Lann Pitchford Group GREPHE Laboratoir ds Plasmas t Convrsion d Enrgi Univrsité d Toulous t CNRS UMR 5213 pitchford@laplac.univ-tls.fr JP Bouf, G. Haglaar, Th Callgari

More information

Carriers Concentration, Current & Hall Effect in Semiconductors. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India

Carriers Concentration, Current & Hall Effect in Semiconductors. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India Carriers Concentration, Current & Hall Effect in Semiconductors 1 Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India http://folk.uio.no/ravi/semi2013 Conductivity Charge

More information

Supplementary Materials

Supplementary Materials 6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic

More information

Compton Scattering. There are three related processes. Thomson scattering (classical) Rayleigh scattering (coherent)

Compton Scattering. There are three related processes. Thomson scattering (classical) Rayleigh scattering (coherent) Comton Scattring Tr ar tr rlatd rocsss Tomson scattring (classical) Poton-lctron Comton scattring (QED) Poton-lctron Raylig scattring (cornt) Poton-atom Tomson and Raylig scattring ar lasticonly t dirction

More information

ECE 344 Microwave Fundamentals

ECE 344 Microwave Fundamentals ECE 44 Microwav Fundamntals Lctur 08: Powr Dividrs and Couplrs Part Prpard By Dr. hrif Hkal 4/0/08 Microwav Dvics 4/0/08 Microwav Dvics 4/0/08 Powr Dividrs and Couplrs Powr dividrs, combinrs and dirctional

More information

Lecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac.

Lecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac. Lctur 2: Discrt-Tim Signals & Systms Rza Mohammadkhani, Digital Signal Procssing, 2015 Univrsity of Kurdistan ng.uok.ac.ir/mohammadkhani 1 Signal Dfinition and Exampls 2 Signal: any physical quantity that

More information

Phys 402: Nonlinear Spectroscopy: SHG and Raman Scattering

Phys 402: Nonlinear Spectroscopy: SHG and Raman Scattering Rquirmnts: Polariation of Elctromagntic Wavs Phys : Nonlinar Spctroscopy: SHG and Scattring Gnral considration of polariation How Polarirs work Rprsntation of Polariation: Jons Formalism Polariation of

More information

Quiz #1 Practice Problem Set

Quiz #1 Practice Problem Set Name: Student Number: ELEC 3908 Physical Electronics Quiz #1 Practice Problem Set? Minutes January 22, 2016 - No aids except a non-programmable calculator - All questions must be answered - All questions

More information

Lecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e

Lecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e 8/7/018 Cours Instructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 3 Skin Dpth & Powr Flow Skin Dpth Ths & Powr nots Flow may contain

More information

Electrons are shared in covalent bonds between atoms of Si. A bound electron has the lowest energy state.

Electrons 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 information

collisions of electrons. In semiconductor, in certain temperature ranges the conductivity increases rapidly by increasing temperature

collisions of electrons. In semiconductor, in certain temperature ranges the conductivity increases rapidly by increasing temperature 1.9. Temperature Dependence of Semiconductor Conductivity Such dependence is one most important in semiconductor. In metals, Conductivity decreases by increasing temperature due to greater frequency of

More information

de/dx Effectively all charged particles except electrons

de/dx Effectively all charged particles except electrons de/dx Lt s nxt turn our attntion to how chargd particls los nrgy in mattr To start with w ll considr only havy chargd particls lik muons, pions, protons, alphas, havy ions, Effctivly all chargd particls

More information

ECE-305: Spring 2018 Final Exam Review

ECE-305: Spring 2018 Final Exam Review C-305: Spring 2018 Final xam Review Pierret, Semiconductor Device Fundamentals (SDF) Chapters 10 and 11 (pp. 371-385, 389-403) Professor Peter Bermel lectrical and Computer ngineering Purdue University,

More information

PN Junction

PN Junction P Junction 2017-05-04 Definition Power Electronics = semiconductor switches are used Analogue amplifier = high power loss 250 200 u x 150 100 u Udc i 50 0 0 50 100 150 200 250 300 350 400 i,u dc i,u u

More information

Lecture-4 Junction Diode Characteristics

Lecture-4 Junction Diode Characteristics 1 Lecture-4 Junction Diode Characteristics Part-II Q: Aluminum is alloyed into n-type Si sample (N D = 10 16 cm 3 ) forming an abrupt junction of circular cross-section, with an diameter of 0.02 in. Assume

More information

PN Junction and MOS structure

PN Junction and MOS structure PN Junction and MOS structure Basic electrostatic equations We will use simple one-dimensional electrostatic equations to develop insight and basic understanding of how semiconductor devices operate Gauss's

More information

Lecture 16 The pn Junction Diode (III)

Lecture 16 The pn Junction Diode (III) Lecture 16 The pn Junction iode (III) Outline I V Characteristics (Review) Small signal equivalent circuit model Carrier charge storage iffusion capacitance Reading Assignment: Howe and Sodini; Chapter

More information

Optoelectronics EE/OPE 451, OPT 444 Fall 2009 Section 1: T/Th 9:30-10:55 PM

Optoelectronics EE/OPE 451, OPT 444 Fall 2009 Section 1: T/Th 9:30-10:55 PM Optolctronics EE/OPE 451, OPT 444 Fall 2009 Sction 1: T/Th 9:30-10:55 PM John D. illiams, Ph.D. Dpartmnt of Elctrical and Computr Enginring 406 Optics Building - UAHuntsvill, Huntsvill, AL 35899 Ph. (256)

More information

Physics 2D Lecture Slides Lecture 12: Jan 28 th 2004

Physics 2D Lecture Slides Lecture 12: Jan 28 th 2004 Brian Wcht, th TA, is away this wk. I will substitut for his offic hours (in my offic 3314 Mayr Hall, discussion and PS sssion. Pl. giv all rgrad rqusts to m this wk (only) Quiz 3 Will Covr Sctions.1-.5

More information

Theory and Applications of Transmission Lines

Theory and Applications of Transmission Lines Thory and Applications of Transmission ins 1 Introduction Typs Topics Gnral Transmission-in Equations Wav Charactristics on Finit Transmission ins Wavguids Optical Fibr 2 Transmission ins Usd for guiding

More information

Sample Exam # 2 ECEN 3320 Fall 2013 Semiconductor Devices October 28, 2013 Due November 4, 2013

Sample Exam # 2 ECEN 3320 Fall 2013 Semiconductor Devices October 28, 2013 Due November 4, 2013 Sample Exam # 2 ECEN 3320 Fall 203 Semiconductor Devices October 28, 203 Due November 4, 203. Below is the capacitance-voltage curve measured from a Schottky contact made on GaAs at T 300 K. Figure : Capacitance

More information

Organic Electronic Devices

Organic 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 information

2. Laser physics - basics

2. Laser physics - basics . Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"

More information

Extraction of Doping Density Distributions from C-V Curves

Extraction of Doping Density Distributions from C-V Curves Extraction of Doping Dnsity Distributions from C-V Curvs Hartmut F.-W. Sadrozinski SCIPP, Univ. California Santa Cruz, Santa Cruz, CA 9564 USA 1. Connction btwn C, N, V Start with Poisson quation d V =

More information

λ = 2L n Electronic structure of metals = 3 = 2a Free electron model Many metals have an unpaired s-electron that is largely free

λ = 2L n Electronic structure of metals = 3 = 2a Free electron model Many metals have an unpaired s-electron that is largely free 5.6 4 Lctur #4-6 pag Elctronic structur of mtals r lctron modl Many mtals av an unpaird s-lctron tat is largly fr Simplst modl: Particl in a box! or a cubic box of lngt L, ψ ( xyz) 8 xπ ny L L L n x π

More information

CS 152 Computer Architecture and Engineering

CS 152 Computer Architecture and Engineering CS 152 Computr Architctur and Enginring Lctur 11 VLSI I 2005-2-22 John Lazzaro (www.cs.brkly.du/~lazzaro) TAs: Td Hong and David Marquardt www-inst.cs.brkly.du/~cs152/ Last Tim: Piplin Hazard Rsolution

More information

Toward a 1D Device Model Part 2: Material Fundamentals

Toward a 1D Device Model Part 2: Material Fundamentals Toward a 1D Device Model Part 2: Material Fundamentals Lecture 8 10/4/2011 MIT Fundamentals of Photovoltaics 2.626/2.627 Fall 2011 Prof. Tonio Buonassisi 1 2.626/2.627 Roadmap You Are Here 2 2.626/2.627:

More information

Gamma-ray burst spectral evolution in the internal shock model

Gamma-ray burst spectral evolution in the internal shock model Gamma-ray burst spctral volution in th intrnal shock modl in collaboration with: Žljka Marija Bošnjak Univrsity of Rijka, Croatia Frédéric Daign (Institut d Astrophysiqu d Paris) IAU$Symposium$324$0$Ljubljana,$Sptmbr$2016$

More information

Model neurons!!the membrane equation!

Model neurons!!the membrane equation! Modl nurons!!th bran quation! Suggstd rading:! Chaptr 5.1-5.3 in Dayan, P. & Abbott, L., Thortical Nuroscinc, MIT Prss, 2001.! Modl nurons: Th bran quation! Contnts:!!!!!! Ion channls Nnst quation Goldan-Hodgkin-Katz

More information

Chapter 6: Polarization and Crystal Optics

Chapter 6: Polarization and Crystal Optics Chaptr 6: Polarization and Crystal Optics * P6-1. Cascadd Wav Rtardrs. Show that two cascadd quartr-wav rtardrs with paralll fast axs ar quivalnt to a half-wav rtardr. What is th rsult if th fast axs ar

More information

We are IntechOpen, the first native scientific publisher of Open Access books. International authors and editors. Our authors are among the TOP 1%

We are IntechOpen, the first native scientific publisher of Open Access books. International authors and editors. Our authors are among the TOP 1% W ar IntcOpn, t first nativ scintific publisr of Opn Accss books 3,35 8,.7 M Opn accss books availabl Intrnational autors and ditors Downloads Our autors ar among t 5 Countris dlivrd to TOP % most citd

More information

Electric (Rocket) Propulsion. EP Overview

Electric (Rocket) Propulsion. EP Overview Elctric (Rockt) Propulsion EP Ovrviw Elctric Propulsion-1 Basics Rockt Propulsion Elmnts Propllant Enrgy Sourc Storag Fd Systm sam in chmical rockts Storag Convrsion Acclrator Elctric Propulsion- 1 Elctric

More information

Calculus II (MAC )

Calculus II (MAC ) Calculus II (MAC232-2) Tst 2 (25/6/25) Nam (PRINT): Plas show your work. An answr with no work rcivs no crdit. You may us th back of a pag if you nd mor spac for a problm. You may not us any calculators.

More information

Additional Math (4047) Paper 2 (100 marks) y x. 2 d. d d

Additional Math (4047) Paper 2 (100 marks) y x. 2 d. d d Aitional Math (07) Prpar b Mr Ang, Nov 07 Fin th valu of th constant k for which is a solution of th quation k. [7] Givn that, Givn that k, Thrfor, k Topic : Papr (00 marks) Tim : hours 0 mins Nam : Aitional

More information

Chapter 6 Solar Cells (Supplementary)

Chapter 6 Solar Cells (Supplementary) 1 Chapter 6 olar Cells (upplementary) Chapter 6... 1 olar Cells... 1 6.1.1... 6.1.... 6.1.3... 6.1.4 Effect of Minority Electron Lifetime on Efficiency... 6.1.5 Effect of Minority hole Lifetime on Efficiency...

More information

MODELING THE FUNDAMENTAL LIMIT ON CONVERSION EFFICIENCY OF QD SOLAR CELLS

MODELING THE FUNDAMENTAL LIMIT ON CONVERSION EFFICIENCY OF QD SOLAR CELLS MODELING THE FUNDAMENTAL LIMIT ON CONVERSION EFFICIENCY OF QD SOLAR CELLS Ա.Մ.Կեչիյանց Ara Kechiantz Institute of Radiophysics and Electronics (IRPhE), National Academy of Sciences (Yerevan, Armenia) Marseille

More information

Charge Carriers in Semiconductor

Charge Carriers in Semiconductor Charge Carriers in Semiconductor To understand PN junction s IV characteristics, it is important to understand charge carriers behavior in solids, how to modify carrier densities, and different mechanisms

More information

Chapter 6 Current and Resistance

Chapter 6 Current and Resistance Chaptr 6 Currnt and Rsistanc 6.1 Elctric Currnt... 1 6.1.1 Currnt Dnsity... 1 6. Ohm s Law... 3 6.3 Elctrical Enrgy and Powr... 6 6.4 Summary... 6.5 Solvd Problms... 8 6.5.1 Rsistivity of a Cabl... 8 6.5.

More information

Solid State Theory Physics 545 Band Theory III

Solid State Theory Physics 545 Band Theory III Solid Stat Thory Physics 545 Band Thory III ach atomic orbital lads to a band of allowd stats in th solid Band of allowd stats Gap: no allowd stats Band of allowd stats Gap: no allowd stats Band of allowd

More information

Thermionic 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 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 information

Lecture 15 The pn Junction Diode (II)

Lecture 15 The pn Junction Diode (II) Lecture 15 The pn Junction Diode (II I-V characteristics Forward Bias Reverse Bias Outline Reading Assignment: Howe and Sodini; Chapter 6, Sections 6.4-6.5 6.012 Spring 2007 Lecture 15 1 1. I-V Characteristics

More information

EE243 Advanced Electromagnetic Theory Lec # 23 Scattering and Diffraction. Reading: Jackson Chapter , lite

EE243 Advanced Electromagnetic Theory Lec # 23 Scattering and Diffraction. Reading: Jackson Chapter , lite Applid M Fall 6, Nuruthr Lctur #3 Vr /5/6 43 Advancd lctromagntic Thory Lc # 3 cattring and Diffraction calar Diffraction Thory Vctor Diffraction Thory Babint and Othr Principls Optical Thorm ading: Jackson

More information

Studying Anomalous Open-Circuit Voltage Drop-Out in Concentrated Photovoltaics Using Computational Numerical Analysis

Studying Anomalous Open-Circuit Voltage Drop-Out in Concentrated Photovoltaics Using Computational Numerical Analysis Studying Anomalous Open-Circuit Voltage Drop-Out in Concentrated Photovoltaics Using Computational Numerical Analysis Margaret A. Stevens, Chandler Downs, David Emerson, James Adler, Scott Maclachlan and

More information

Novel Inorganic-Organic Perovskites for Solution Processed Photovoltaics. PIs: Mike McGehee and Hema Karunadasa

Novel Inorganic-Organic Perovskites for Solution Processed Photovoltaics. PIs: Mike McGehee and Hema Karunadasa Novel Inorganic-Organic Perovskites for Solution Processed Photovoltaics PIs: Mike McGehee and Hema Karunadasa 1 Perovskite Solar Cells are Soaring Jul 2013 Grätzel, EPFL 15% Nov 2014 KRICT 20.1%! Seok,

More information

PHYS ,Fall 05, Term Exam #1, Oct., 12, 2005

PHYS ,Fall 05, Term Exam #1, Oct., 12, 2005 PHYS1444-,Fall 5, Trm Exam #1, Oct., 1, 5 Nam: Kys 1. circular ring of charg of raius an a total charg Q lis in th x-y plan with its cntr at th origin. small positiv tst charg q is plac at th origin. What

More information

3 Minority carrier profiles (the hyperbolic functions) Consider a

3 Minority carrier profiles (the hyperbolic functions) Consider a Microelectronic Devices and Circuits October 9, 013 - Homework #3 Due Nov 9, 013 1 Te pn junction Consider an abrupt Si pn + junction tat as 10 15 acceptors cm -3 on te p-side and 10 19 donors on te n-side.

More information

ECE-305: Fall 2016 Minority Carrier Diffusion Equation (MCDE)

ECE-305: Fall 2016 Minority Carrier Diffusion Equation (MCDE) ECE-305: Fall 2016 Minority Carrier Diffusion Equation (MCDE) Professor Peter Bermel Electrical and Computer Engineering Purdue University, West Lafayette, IN USA pbermel@purdue.edu Pierret, Semiconductor

More information

Outline. Solar Photovoltaic Applications. Midterm Problem One. Midterm Results. Midterm Problem Two. Midterm Problem One II

Outline. Solar Photovoltaic Applications. Midterm Problem One. Midterm Results. Midterm Problem Two. Midterm Problem One II Photovoltaic Solar April 6, 010 Solar Photovoltaic Application Larry Cartto Mchanical Enginring 483 Altrnativ Enrgy Enginring II April 6, 010 Outlin Midtrm xam rult Mt on Wdnday at PPM Confrnc room for

More information

Chapter 2. Electronics I - Semiconductors

Chapter 2. Electronics I - Semiconductors Chapter 2 Electronics I - Semiconductors Fall 2017 talarico@gonzaga.edu 1 Charged Particles The operation of all electronic devices is based on controlling the flow of charged particles There are two type

More information

Semiconductor Physics fall 2012 problems

Semiconductor Physics fall 2012 problems Semiconductor Physics fall 2012 problems 1. An n-type sample of silicon has a uniform density N D = 10 16 atoms cm -3 of arsenic, and a p-type silicon sample has N A = 10 15 atoms cm -3 of boron. For each

More information

Semiconductor Junctions

Semiconductor Junctions 8 Semiconductor Junctions Almost all solar cells contain junctions between different materials of different doping. Since these junctions are crucial to the operation of the solar cell, we will discuss

More information