Ellipsometry Overview

Size: px
Start display at page:

Download "Ellipsometry Overview"

Transcription

1 llpsometry Overvew ~ R Δ p ρ = ta( Ψ) e = ~ Rs ñ(λ) = (λ) + k(λ) ε = ñ 2 p-plae s-plae p-plae plae of cdece s-plae

2 llpsometry buldg-blocks Lght ad Polarzato Materals / Optcal Costats Iteracto of Lght wth Materals llpsometry Procedure Measuremet Aalyss

3 lectromagetc Plae Wave Lght From Maxwell s equatos we ca descrbe a plae wave X 2π ( z, t) = 0 s ( z vt) + ξ λ ampltude l wavelegth velocty arbtrary phase Y lectrc feld, (z,t) Magetc feld, B(z,t) Z Drecto of propagato

4 Lght Lght Frequecy of wave remas the same Velocty ad wavelegth vary dfferet materals υ = v λ c v = ergy of photo ( ev speed speed of of lght lght ) = hυ = 1 = 2 1,240 λ ( m ) Plack s Plack s costat costat

5 Itesty ad Polarzato Lght Itesty = Sze of lectrc feld. I 2 Polarzato = Shape of lectrc feld travel. Y Less Itese Dfferet Sze (Itesty) More Itese Y X Same Shape! (Polarzato) X

6 Learly Polarzed Lght Lght X ad Y propagate same drecto -felds orthogoal; waves -phase Result: learly polarzed wave the 'plae of vbrato' depeds o ampltudes of x & Y X wave1 Y wave2 Z

7 Crcularly Polarzed Lght Lght x ad Y have: equal ampltude X wave1 90 out of phase Y wave2 Z

8 llptcally Polarzed Lght Lght x ad Y have arbtrary phase ad ampltude Result s ellptcal X wave1 Y wave2 Z

9 Optcal Costats Materal Complex Refractve Idex: ñ= + k Descrbes what materal does to lght wave. Alteratvely Complex Delectrc Fucto:ε= ε 1 + ε 2 Descrbes what lght does to materal. ε 1 = volume polarzato term ε 2 = volume absorpto ε = ñ 2

10 Complex Refractve Idex Materal (λ) = Refractve Idex ñ(λ) = (λ) + k(λ) Descrbes wave velocty ad refracto. k(λ) = xtcto Coeffcet Descrbes loss of eergy.

11 Kramers-Krog Relato Materal Real ad magary parts deped o each other. ε 1 ε 2 Absorpto causes aomalous dsperso. k Frequecy (eergy)

12 Optcal Costats Materal Absorpto by dfferet mechasms: Free-carrer, lattce ad molecular vbrato, electroc trasto IR UV

13 Trasparet Rego Materal Idex decreases for loger wavelegths. Hgher dex whe close to large absorpto. Idex, SO2 S3N4 S Wavelegth m

14 Delectrc Materal lectrc feld causes oscllatg electro charge cloud. Photo I lectros move easly, atomc core too heavy to move. Dsplaced charge = lectrc Dpoles.

15 Delectrc Materal Atoms borrow eergy from electrc feld. The gve t back wth NO LOSS. DIPOL RADIATION! Oscllatg Dpole New Photo Out! - Same Frequecy - Same ergy = hν

16 Delectrc Materal Oscllatos take tme Re-emtted wave s delayed. I Phase Out of Phase Referece Wave Wave has bee slowed Idex, = (speed vod)/(speed materal)

17 Absorbg Rego Materal lectrc feld loses eergy to a process materal lectroc Trasto Lattce Vbrato Molecular Vbrato Free-carrer

18 lectroc Trasto Materal lectros eergy bads. Gap betwee valece ad coducto bad. If photo has eergy larger tha gap, electro ca excte to hgher state.

19 lectroc Trasto Materal ergy bads ca be very complcated wth dfferet acceptable trastos (drect or drect). S. Adach, Optcal propertes of crystalle ad amorphous semcoductors, Kluwer Academc Publshers, Bosto (1999).

20 lectroc Trasto Materal Absorpto for each trasto. 1.2 Imag(Delectrc Costat), ε Slco GaAs ε Idrect gap S GaAs Drect gap Photo ergy (ev) Photo ergy (ev)

21 Amorphous or Crystalle Materal lectroc trastos broadeed for amorphous materals.

22 Molecular Vbrato Materal lectrc Feld wth slow frequecy (IR) ca vbrate molecules (stretch or bed). CH2 stretch (symmetrc) CH2 stretch (asymmetrc) N-H stretch C=O stretch

23 Lattce Vbratos Materal lectrc Feld causes lattce to vbrate Logtudal (LO) or Trasverse (TO) Optcal 180 TO 2TO TO+LO k Δ degrees TO+LA Wave Number (cm -1 )

24 Free-carrers Materal Metals have more electros tha eeded for bodg (covalet bods = sharg electros). lectrc feld causes free electros to move! Wave eergy lost as heat.

25 Free-carrers Materal Absorb strogly for low frequecy electrc feld k creases toward IR Idex of refracto, k Nckel Wavelegth (m) xtcto Coeffcet, k Idex of refracto, k Alumum xtcto Coeffcet, k Wavelegth (m)

26 Optcal Costat Summary Materal Trasparet rego: dex decreases toward loger wavelegths (ormal dsperso) Absorbg rego: KK cosstecy creates aomalous dsperso Dfferet absorbg mechasms cosdered.

27 Lght at terface Iteracto Reflectos caused by dex dfferece: Normal cdece: Oblque Icdece Refracto Reflecto Ñ 1 s φ 1 = Ñ 2 s φ 2 R = ( ) 1 2 ( + ) dex, Ñ 1 velocty, c φ 1 φ 1 φ = φ r dex, Ñ 2 velocty, v φ 2

28 Plae of Icdece Iteracto lectrc feld ether parallel (p) or perpedcular (s) to plae of cdece. Plae of Icdece defed by: p p Icdet Ray s p s Sample Normal Reflected Ray s plae of cdece

29 Iteracto Polarzed Reflecto P- ad S- waves do ot mx (sotropc-case) Materal dfferetates betwee p- ad s- lght Rp Rs Reflecto Agle of Icdece ( )

30 Fresel Coeffcets Descrbe reflecto ad trasmsso at terface: Deped o agle ad polarzato drecto (p or s) t t t t p r p r θ θ θ θ cos cos cos cos = = t t t t s r s r θ θ θ θ cos cos cos cos = = t t s t s t θ θ θ cos cos cos = = t t p t p t θ θ θ cos cos cos = = Iteracto

31 Th Flm Iterferece Iteracto r tot = -2β -4β r01 + t01r12t10e + t01r12 r10t10e r 01 t 01 r 12 t 10e -2β FILM PHAS THICKNSS ~ 0 ~ 1 t 01 r 12 r 10 r 12 t 10 e -4β β = d1 2π 1 cos θ 1 λ ~ 2

32 llpsometry Measuremet Iteracto Measures chage polarzato of reflected lght. Sample s defed by reflecto of p- ad s- polarzed lght. p s out = ~ R 0 p 0 ~ R ~ R Δ p ρ = ta( ψ ) e = ~ Rs s p s p-plae s-plae plae of cdece p-plae s-plae ρ = Re( ρ) + Im(ρ ) = ta(ψ)cos( Δ) + ta(ψ)s(δ) = ta(ψ)e Δ = R p R s e (δ p δ s ) =?R p?r s

33 What ca S determe? llpsometry Measures: Propertes of Iterest: Flm Thckess Refractve Idex Ps (Ψ) Delta (Δ) Surface Roughess Iterfacal Mxg Composto Crystallty Asotropy Uformty

34 What I Stu llpsometry Measures Substrate temperature Substrate surface qualty Oxde thckess ad desorpto Iterfacal regos Growth ad etch rates Substrate ad flm optcal costats (before surface oxdato) Idex gradets Alloy composto Multple-layer thckesses

Absorption in Solar Atmosphere

Absorption in Solar Atmosphere Absorpto Solar Atmosphere A black body spectrum emtted from solar surface causes exctato processes o atoms the solar atmosphere. Ths tur causes absorpto of characterstc wavelegths correspodg to those atoms

More information

Periodic Table of Elements. EE105 - Spring 2007 Microelectronic Devices and Circuits. The Diamond Structure. Electronic Properties of Silicon

Periodic Table of Elements. EE105 - Spring 2007 Microelectronic Devices and Circuits. The Diamond Structure. Electronic Properties of Silicon EE105 - Srg 007 Mcroelectroc Devces ad Crcuts Perodc Table of Elemets Lecture Semcoductor Bascs Electroc Proertes of Slco Slco s Grou IV (atomc umber 14) Atom electroc structure: 1s s 6 3s 3 Crystal electroc

More information

The E vs k diagrams are in general a function of the k -space direction in a crystal

The E vs k diagrams are in general a function of the k -space direction in a crystal vs dagram p m m he parameter s called the crystal mometum ad s a parameter that results from applyg Schrödger wave equato to a sgle-crystal lattce. lectros travelg dfferet drectos ecouter dfferet potetal

More information

Evolution Operators and Boundary Conditions for Propagation and Reflection Methods

Evolution Operators and Boundary Conditions for Propagation and Reflection Methods voluto Operators ad for Propagato ad Reflecto Methods Davd Yevck Departmet of Physcs Uversty of Waterloo Physcs 5/3/9 Collaborators Frak Schmdt ZIB Tlma Frese ZIB Uversty of Waterloo] atem l-refae Nortel

More information

Reflection and transmission of light at a curved interface: coherent state approach. N.I. Petrov

Reflection and transmission of light at a curved interface: coherent state approach. N.I. Petrov Reflecto ad trasmsso of lght at a curved terface: coheret state approach N.I. Petrov Lea Street, 9-39, Istra, Moscow Rego 435, Russa Phase-space procedure based o coheret state represetato s proposed for

More information

UNIVERSITY OF CALIFORNIA, BERKELEY DEPARTMENT OF ELECTRICAL ENGINEERING AND COMPUTER SCIENCES. Midterm I

UNIVERSITY OF CALIFORNIA, BERKELEY DEPARTMENT OF ELECTRICAL ENGINEERING AND COMPUTER SCIENCES. Midterm I UNIVERSITY OF CALIFORNIA, BERKELEY EPARTMENT OF ELECTRICAL ENGINEERING AN COMPUTER SCIENCES EECS 130 Professor Chemg Hu Fall 009 Mdterm I Name: Closed book. Oe sheet of otes s allowed. There are 8 pages

More information

6.4.5 MOS capacitance-voltage analysis

6.4.5 MOS capacitance-voltage analysis 6.4.5 MOS capactace-voltage aalyss arous parameters of a MOS devce ca be determed from the - characterstcs.. Type of substrate dopg. Isulator capactace = /d sulator thckess d 3. The mmum depleto capactace

More information

X-ray vortices from nonlinear inverse Thomson scattering

X-ray vortices from nonlinear inverse Thomson scattering JLab semar 8/7/6 X-ray vortces from olear verse Thomso scatterg Yoshtaka Tara Natoal Isttute of Advaced Idustral Scece ad Techology (AIST) Vstg scetst: Msssspp State Uversty ad Jefferso Lab. Optcal vortex

More information

Optical Design with Zemax for PhD

Optical Design with Zemax for PhD Optcal Desg wth Zemax for PhD Lecture 16: Coatgs 16-5-13 Herbert Gross Wter term 15 / Summer term 16 www.ap.u-ea.de Prelmary Schedule No Date Subect Detaled cotet 1 11.11. Itroducto Zemax terface, meus,

More information

Layered structures: transfer matrix formalism

Layered structures: transfer matrix formalism Layered tructure: trafer matrx formalm Iterface betwee LI meda Trafer matrx formalm Petr Kužel Practcally oly oe formula to be kow order to calculate ay tructure Applcato: Atreflectve coatg Delectrc mrror,

More information

Homework #2 Solutions, EE/MSE 486, Spring 2017 Problem 1:

Homework #2 Solutions, EE/MSE 486, Spring 2017 Problem 1: Homework # Solutos, EE/MSE 486, Sprg 017 Problem 1: P o p N N A ( N N A) Here / for type dopg; 4 p p N A N ( N A N) / for p type dog. 4 At 1000C, 3.1*10 16 3/ From the table the otes, we have T 0.603eV

More information

MODELING AND OPTIMIZATION OF TWO-LAYER POROUS ASPHALT ROADS ABSTRACT 1- INTRODUCTION

MODELING AND OPTIMIZATION OF TWO-LAYER POROUS ASPHALT ROADS ABSTRACT 1- INTRODUCTION 143.DOC/1 MODELING AND OPTIMIZATION OF TWO-LAYER POROUS ASPHALT ROADS A. KUIJPERS, G. VAN BLOKLAND M+P Nose & Vbrato Cosultats, Brustesgel 3, NL-531 AD's, Hertogebosch, Netherlads Tél.: +31 73 648851 /

More information

Block-Based Compact Thermal Modeling of Semiconductor Integrated Circuits

Block-Based Compact Thermal Modeling of Semiconductor Integrated Circuits Block-Based Compact hermal Modelg of Semcoductor Itegrated Crcuts Master s hess Defese Caddate: Jg Ba Commttee Members: Dr. Mg-Cheg Cheg Dr. Daqg Hou Dr. Robert Schllg July 27, 2009 Outle Itroducto Backgroud

More information

Probing the Electronic Structure of Solids by Angle Resolved Photoemission Spectroscopy (ARPES) workshop April 2016, IPM-Tehran

Probing the Electronic Structure of Solids by Angle Resolved Photoemission Spectroscopy (ARPES) workshop April 2016, IPM-Tehran Probg the Electroc Structure of Solds by Agle Resolved Photoemsso Spectroscopy (ARPES) workshop 5-6 Aprl 016, IPM-Tehra Alakbar Ghafar Helmholtz-Zetrum Berl (HZB), EM-AMCT HZB: BESSY II- Reactor BER II

More information

Space charge. Lecture 8 09/11/2011. p-n junction with gradient. p-n junction with gradient. V. p-n junction. Space charge

Space charge. Lecture 8 09/11/2011. p-n junction with gradient. p-n junction with gradient. V. p-n junction. Space charge ecture 8 09/11/011 Sace charge. - jucto Sace charge th a gradet Out of equlbrum Sace charge -tye ad -tye regos Usually N >>N A thus q N x = N A /(N +N A x = N /(N +N A A ad x = The sace charge exteds towards

More information

Semiconductor Device Physics

Semiconductor Device Physics 1 Semcoductor evce Physcs Lecture 7 htt://ztomul.wordress.com 0 1 3 Semcoductor evce Physcs Chater 6 Jucto odes: I-V Characterstcs 3 Chater 6 Jucto odes: I-V Characterstcs Qualtatve ervato Majorty carrers

More information

III-16 G. Brief Review of Grand Orthogonality Theorem and impact on Representations (Γ i ) l i = h n = number of irreducible representations.

III-16 G. Brief Review of Grand Orthogonality Theorem and impact on Representations (Γ i ) l i = h n = number of irreducible representations. III- G. Bref evew of Grad Orthogoalty Theorem ad mpact o epresetatos ( ) GOT: h [ () m ] [ () m ] δδ δmm ll GOT puts great restrcto o form of rreducble represetato also o umber: l h umber of rreducble

More information

Stress Wave propagation in Electro-Magneto-Elastic plate of arbitrary cross-sections

Stress Wave propagation in Electro-Magneto-Elastic plate of arbitrary cross-sections Iteratoal Joural of Scetfc & Egeerg Research Volume 3, Issue 8, August-1 1 ISSN 9-5518 Stress Wave propagato Electro-Mageto-Elastc plate of arbtrary cross-sectos P. Pousamy Departmet of Mathematcs Govermet

More information

Optical Design with Zemax for PhD - Basics

Optical Design with Zemax for PhD - Basics Optcal Desg wth Zema for PhD - Bascs Semar 5 : Phscal Modellg II 4-- Herbert Gross Wter term 4 www.ap.u-jea.de Prelmar Schedule No Date Subject Detaled cotet.. Repetto Correcto, hadlg, mult-cofgurato 9..

More information

Physical Optics. Lecture 12: Polarization Herbert Gross.

Physical Optics. Lecture 12: Polarization Herbert Gross. Phscal Optcs Lecture : Polarato 7-5-3 Herbert Gross www.ap.u-jea.de Phscal Optcs: Cotet No Date Subject Ref Detaled Cotet 5.4. Wave optcs G Comple felds, wave equato, k-vectors, terferece, lght propagato,

More information

Modeling and analysis of waves in a heat conducting thermo-elastic plate of elliptical shape

Modeling and analysis of waves in a heat conducting thermo-elastic plate of elliptical shape 589 Modelg ad aalyss of waves a heat coductg thermo-elastc plate of ellptcal shape Abstract Wave propagato heat coductg thermo elastc plate of ellptcal cross-secto s studed usg the Fourer expaso collocato

More information

Cross-plane Seebeck coefficient and Lorenz number in superlattices

Cross-plane Seebeck coefficient and Lorenz number in superlattices PHYSICAL REVIEW B 76, 25311 27 Cross-plae Seebeck coeffcet ad Lorez umber superlattces Z. Ba, M. Zebarjad, R. Sgh, Y. Ezzahr, ad A. Shakour Electrcal Egeerg Departmet, Uversty of Calfora, Sata Cruz, Calfora

More information

Phys 102 Lecture 25 The quantum mechanical model of light

Phys 102 Lecture 25 The quantum mechanical model of light Phys 102 Lecture 25 The quatum mechaical model of light 1 Recall last time Problems with classical physics Stability of atoms Atomic spectra Photoelectric effect Quatum model of the atom Bohr model oly

More information

MOLECULAR VIBRATIONS

MOLECULAR VIBRATIONS MOLECULAR VIBRATIONS Here we wsh to vestgate molecular vbratos ad draw a smlarty betwee the theory of molecular vbratos ad Hückel theory. 1. Smple Harmoc Oscllator Recall that the eergy of a oe-dmesoal

More information

1. MOS: Device Operation and Large Signal Model

1. MOS: Device Operation and Large Signal Model 1. MOS: ece Oerato ad arge Sgal Model Readg: Sedra & Smth Sec. 5.1-5.3 (S&S 5 th Ed: Sec. 4.1-4.3) ECE 10, Fall 011, F. Najmabad Oeratoal Bass of a Feld-Effect Trasstor (1) Cosder the hyothetcal semcoductor

More information

) 12 = 1+ j. = ε 2. = n 2 n 1. sinθ ic. mπ a. = 1+ j. cos mπ a x. H z. =±j ε 2. sin 2 θ i. cosθ t 1 [3.31] ε 2ε1. θ i. ε =1e jφ. tan φ sin 2.

) 12 = 1+ j. = ε 2. = n 2 n 1. sinθ ic. mπ a. = 1+ j. cos mπ a x. H z. =±j ε 2. sin 2 θ i. cosθ t 1 [3.31] ε 2ε1. θ i. ε =1e jφ. tan φ sin 2. Mawell s Equatos (geeral deretal E B D ρ H J + D B 0 Mawell s Equatos (tme harmoc E jωb D ρ [.a] [.b] [.c] [.d] [.a] [.b] H J + D [.c] B 0 [.d] Mawell s Equatos (tegral E dl B ds [.] D ds ρdv V [.] D H

More information

2018 TIGP: Advanced Nanotechnology (A) Part 1: Photonic Crystals and Devices

2018 TIGP: Advanced Nanotechnology (A) Part 1: Photonic Crystals and Devices 08 TIGP: Advaced Naotecholog A Part : Photoc Crstals ad Devces Lecture # M-Hsug Shh Research Ceter for Appled Sceces RCAS Academa Sca Tawa Mar. 4 08 Comparso of Quatum Mechacs ad lectrdamcs Table teded

More information

Reflection of Plane Waves from a Free Surface of an Initially Stressed Transversely Isotropic Dissipative Medium

Reflection of Plane Waves from a Free Surface of an Initially Stressed Transversely Isotropic Dissipative Medium ppled Mathematcs 0 9- do:0.6/am.0.956 Publshed Ole September 0 (http://www.scrp.org/joural/am) Reflecto of Plae Waves from a Free Surface of a Itally Stressed Trasversely Isotropc Dsspatve Medum bstract

More information

Physical Optics. Lecture 7: Polarization Herbert Gross.

Physical Optics. Lecture 7: Polarization Herbert Gross. Phscal Optcs Lecture 7: Polarato 8--6 Herbert Gross www.ap.u-jea.de Phscal Optcs: Cotet No Date Subject Ref Detaled Cotet 8.. Wave optcs G Comple felds, wave equato, k-vectors, terferece, lght propagato,

More information

ELECTRON HEATING IN THE CONDUCTION BAND OF INSULATORS UNDER FEMTOSECOND LASER PULSE IRRADIATION

ELECTRON HEATING IN THE CONDUCTION BAND OF INSULATORS UNDER FEMTOSECOND LASER PULSE IRRADIATION LCTRON HATING IN TH CONDUCTION BAND OF INSULATORS UNDR FMTOSCOND LASR PULS IRRADIATION Ilya Bogatyrev H. Bacau A.N. Belsy I.B. Bogatyrev J. Gaud G. Geoffroy S. Guzard P. Mart Yu.V. Popov A.N. Vasl ev B.N.

More information

ECE 595, Section 10 Numerical Simulations Lecture 19: FEM for Electronic Transport. Prof. Peter Bermel February 22, 2013

ECE 595, Section 10 Numerical Simulations Lecture 19: FEM for Electronic Transport. Prof. Peter Bermel February 22, 2013 ECE 595, Secto 0 Numercal Smulatos Lecture 9: FEM for Electroc Trasport Prof. Peter Bermel February, 03 Outle Recap from Wedesday Physcs-based devce modelg Electroc trasport theory FEM electroc trasport

More information

Module 1 : The equation of continuity. Lecture 5: Conservation of Mass for each species. & Fick s Law

Module 1 : The equation of continuity. Lecture 5: Conservation of Mass for each species. & Fick s Law Module : The equato of cotuty Lecture 5: Coservato of Mass for each speces & Fck s Law NPTEL, IIT Kharagpur, Prof. Sakat Chakraborty, Departmet of Chemcal Egeerg 2 Basc Deftos I Mass Trasfer, we usually

More information

Binary plasmonic waveguide arrays. Modulational instability and gap solitons.

Binary plasmonic waveguide arrays. Modulational instability and gap solitons. Bary plasmoc wavegude arrays. Modulatoal stablty ad gap soltos. Aldo Audtore Matteo Cofort Costato De Agels Dpartmeto d Igegera dell Iformaoe Uverstà degl Stud d Bresca Alejadro B. Aceves Souther Methodst

More information

Diode DC Non-ideal Characteristics

Diode DC Non-ideal Characteristics Dode DC No-deal Characterstcs - e qv/kt V reverse curret ot saturated (geerato the deleto rego) dode breakdow 2 3 recombato the deleto rego l( ) 5 hgh-level jecto of morty carrers l( ) sloeq/ηkt V η η2

More information

Physics 114 Exam 2 Fall Name:

Physics 114 Exam 2 Fall Name: Physcs 114 Exam Fall 015 Name: For gradg purposes (do ot wrte here): Questo 1. 1... 3. 3. Problem Aswer each of the followg questos. Pots for each questo are dcated red. Uless otherwse dcated, the amout

More information

Summary of the lecture in Biostatistics

Summary of the lecture in Biostatistics Summary of the lecture Bostatstcs Probablty Desty Fucto For a cotuos radom varable, a probablty desty fucto s a fucto such that: 0 dx a b) b a dx A probablty desty fucto provdes a smple descrpto of the

More information

Organic Electronic Devices

Organic Electronic Devices Orgac Electroc Devces Week 1: Semcoductor Sythess ad Characterzato Lecture 1.1: A Itroducto to Orgac Electroc aterals Brya W. Boudours Chemcal Egeerg Purdue Uversty 1 Lecture Overvew ad Learg Objectves

More information

Theory study about quarter-wave-stack dielectric mirrors

Theory study about quarter-wave-stack dielectric mirrors Theor tud about quarter-wave-tack delectrc rror Stratfed edu tratted reflected reflected Stratfed edu tratted cdet cdet T T Frt, coder a wave roagato a tratfed edu. A we kow, a arbtrarl olared lae wave

More information

Carrier Action under Perturbation

Carrier Action under Perturbation Carrer Acto uder Perturbato Eulbrum: o curret ad o formato ca be represeted. Ferm-level s flat! Perturbato s ecessary to artfcally ecode formato perturbed states: electrc feld (drft), cocetrato gradet

More information

Uniform magnetic susceptibilities

Uniform magnetic susceptibilities Uform magetc susceptbltes Typcal behavors ad measuremet techques SUSCPTIILIT UNIFORM & MAGNTOMTRIS page 1 - M ICFP- lectroc propertes of solds (Fabrce ert Varous behavors of M(H magetzato M Lear respose

More information

ECSE-6300 IC Fabrication Laboratory Lecture 6 Diffusion in Silicon. Lecture Outline

ECSE-6300 IC Fabrication Laboratory Lecture 6 Diffusion in Silicon. Lecture Outline ECSE-6300 IC Fabrcato Laboratory Lecture 6 ffuso Slco Prof. Resselaer Polytechc Isttute Troy, NY 1180 Offce: CII-69 Tel.: (518) 76-909 e-mals: luj@rp.edu http://www.ecse.rp.edu/courses/s16/ecse 6300/dex.html

More information

IJISET - International Journal of Innovative Science, Engineering & Technology, Vol. 2 Issue 9, September 2015.

IJISET - International Journal of Innovative Science, Engineering & Technology, Vol. 2 Issue 9, September 2015. P P P P solar IJISET - Iteratoal Joural of Iovatve Scece, Egeerg & Techology, Vol. Issue 9, September 05. ISSN 348 7968 etermato Of The Jucto Surface recombato Velocty mtg The Ope Crcut (Sfoc) For A Bfacal

More information

C-1: Aerodynamics of Airfoils 1 C-2: Aerodynamics of Airfoils 2 C-3: Panel Methods C-4: Thin Airfoil Theory

C-1: Aerodynamics of Airfoils 1 C-2: Aerodynamics of Airfoils 2 C-3: Panel Methods C-4: Thin Airfoil Theory ROAD MAP... AE301 Aerodyamcs I UNIT C: 2-D Arfols C-1: Aerodyamcs of Arfols 1 C-2: Aerodyamcs of Arfols 2 C-3: Pael Methods C-4: Th Arfol Theory AE301 Aerodyamcs I Ut C-3: Lst of Subects Problem Solutos?

More information

Chapter Two. An Introduction to Regression ( )

Chapter Two. An Introduction to Regression ( ) ubject: A Itroducto to Regresso Frst tage Chapter Two A Itroducto to Regresso (018-019) 1 pg. ubject: A Itroducto to Regresso Frst tage A Itroducto to Regresso Regresso aalss s a statstcal tool for the

More information

best estimate (mean) for X uncertainty or error in the measurement (systematic, random or statistical) best

best estimate (mean) for X uncertainty or error in the measurement (systematic, random or statistical) best Error Aalyss Preamble Wheever a measuremet s made, the result followg from that measuremet s always subject to ucertaty The ucertaty ca be reduced by makg several measuremets of the same quatty or by mprovg

More information

Engineering Vibration 1. Introduction

Engineering Vibration 1. Introduction Egeerg Vbrato. Itroducto he study of the moto of physcal systems resultg from the appled forces s referred to as dyamcs. Oe type of dyamcs of physcal systems s vbrato, whch the system oscllates about certa

More information

MEASURES OF DISPERSION

MEASURES OF DISPERSION MEASURES OF DISPERSION Measure of Cetral Tedecy: Measures of Cetral Tedecy ad Dsperso ) Mathematcal Average: a) Arthmetc mea (A.M.) b) Geometrc mea (G.M.) c) Harmoc mea (H.M.) ) Averages of Posto: a) Meda

More information

Newton s Power Flow algorithm

Newton s Power Flow algorithm Power Egeerg - Egll Beedt Hresso ewto s Power Flow algorthm Power Egeerg - Egll Beedt Hresso The ewto s Method of Power Flow 2 Calculatos. For the referece bus #, we set : V = p.u. ad δ = 0 For all other

More information

Lecture 07: Poles and Zeros

Lecture 07: Poles and Zeros Lecture 07: Poles ad Zeros Defto of poles ad zeros The trasfer fucto provdes a bass for determg mportat system respose characterstcs wthout solvg the complete dfferetal equato. As defed, the trasfer fucto

More information

Objectives of Multiple Regression

Objectives of Multiple Regression Obectves of Multple Regresso Establsh the lear equato that best predcts values of a depedet varable Y usg more tha oe eplaator varable from a large set of potetal predctors {,,... k }. Fd that subset of

More information

Ideal multigrades with trigonometric coefficients

Ideal multigrades with trigonometric coefficients Ideal multgrades wth trgoometrc coeffcets Zarathustra Brady December 13, 010 1 The problem A (, k) multgrade s defed as a par of dstct sets of tegers such that (a 1,..., a ; b 1,..., b ) a j = =1 for all

More information

Statistical characteristics of the normalized Stokes parameters

Statistical characteristics of the normalized Stokes parameters Scece Cha Seres F: Iformato Sceces 008 SCIENCE IN CHINA PRESS Sprger www.sccha.com fo.sccha.com www.sprgerlk.com Statstcal characterstcs of the ormalzed Stokes parameters LIU Tao 1 WANG XueSog 1 & XIAO

More information

EE105 - Fall 2006 Microelectronic Devices and Circuits. Your EECS105 Week

EE105 - Fall 2006 Microelectronic Devices and Circuits. Your EECS105 Week EE15 - Fall 6 Mcroelectroc Devces a Crcuts Prof. Ja M. Rabaey (ja@eecs) Lecture : Semcouctor Bascs Your EECS15 Week Mo Tu We Th Fr 9am 1am Lab 353 Cory Lab 353 Cory Lab 353 Cory 11am Dscusso 93 Cory 1pm

More information

DATE: 21 September, 1999 TO: Jim Russell FROM: Peter Tkacik RE: Analysis of wide ply tube winding as compared to Konva Kore CC: Larry McMillan

DATE: 21 September, 1999 TO: Jim Russell FROM: Peter Tkacik RE: Analysis of wide ply tube winding as compared to Konva Kore CC: Larry McMillan M E M O R A N D U M DATE: 1 September, 1999 TO: Jm Russell FROM: Peter Tkack RE: Aalyss of wde ply tube wdg as compared to Kova Kore CC: Larry McMlla The goal of ths report s to aalyze the spral tube wdg

More information

( ) Thermal noise ktb (T is absolute temperature in kelvin, B is bandwidth, k is Boltzamann s constant) Shot noise

( ) Thermal noise ktb (T is absolute temperature in kelvin, B is bandwidth, k is Boltzamann s constant) Shot noise OISE Thermal oe ktb (T abolute temperature kelv, B badwdth, k Boltzama cotat) 3 k.38 0 joule / kelv ( joule /ecod watt) ( ) v ( freq) 4kTB Thermal oe refer to the ketc eergy of a body of partcle a a reult

More information

2C09 Design for seismic and climate changes

2C09 Design for seismic and climate changes 2C09 Desg for sesmc ad clmate chages Lecture 08: Sesmc aalyss of elastc MDOF systems Aurel Strata, Poltehca Uversty of Tmsoara 06/04/2017 Europea Erasmus Mudus Master Course Sustaable Costructos uder atural

More information

Multiple Choice Test. Chapter Adequacy of Models for Regression

Multiple Choice Test. Chapter Adequacy of Models for Regression Multple Choce Test Chapter 06.0 Adequac of Models for Regresso. For a lear regresso model to be cosdered adequate, the percetage of scaled resduals that eed to be the rage [-,] s greater tha or equal to

More information

THE PHOTON WAVE FUNCTION AND THE FRESNEL FORMULAS

THE PHOTON WAVE FUNCTION AND THE FRESNEL FORMULAS Romaa Reorts Physcs Vol 6 No P 36 368 OPTICS THE PHOTON WAVE FUNCTION AND THE FRESNEL FORMULAS I-IOVITZ POPESCU P STERIAN M DOBRE Natoal Isttute for Lasers Plasmas ad Radato Physcs PO Box MG7 775 Magurele

More information

Signal,autocorrelation -0.6

Signal,autocorrelation -0.6 Sgal,autocorrelato Phase ose p/.9.3.7. -.5 5 5 5 Tme Sgal,autocorrelato Phase ose p/.5..7.3 -. -.5 5 5 5 Tme Sgal,autocorrelato. Phase ose p/.9.3.7. -.5 5 5 5 Tme Sgal,autocorrelato. Phase ose p/.8..6.

More information

Solid State Device Fundamentals

Solid State Device Fundamentals Sold State Devce Fudametals 9 polar jucto trasstor Sold State Devce Fudametals 9. polar Jucto Trasstor NS 345 Lecture ourse by Alexader M. Zatsev alexader.zatsev@cs.cuy.edu Tel: 718 98 81 4N101b Departmet

More information

Stationary states of atoms and molecules

Stationary states of atoms and molecules Statoary states of atos ad olecules I followg wees the geeral aspects of the eergy level structure of atos ad olecules that are essetal for the terpretato ad the aalyss of spectral postos the rotatoal

More information

Simulations of Optical Thin Films

Simulations of Optical Thin Films Dael O Keeffe 7/4/9 Dasy Wllams Smulatos of Optcal Th Flms Th flm terferece, despte eg a terestg physcal pheomea ts ow rght, has umerous applcatos to varous forms of dustry. A few examples are optcal commucato,

More information

On the Link Between the Concepts of Kurtosis and Bipolarization. Abstract

On the Link Between the Concepts of Kurtosis and Bipolarization. Abstract O the Lk etwee the Cocepts of Kurtoss ad polarzato Jacques SILE ar-ila Uversty Joseph Deutsch ar-ila Uversty Metal Haoka ar-ila Uversty h.d. studet) Abstract I a paper o the measuremet of the flatess of

More information

Carbonyl Groups. University of Chemical Technology, Beijing , PR China;

Carbonyl Groups. University of Chemical Technology, Beijing , PR China; Electroc Supplemetary Materal (ESI) for Physcal Chemstry Chemcal Physcs Ths joural s The Ower Socetes 0 Supportg Iformato A Theoretcal Study of Structure-Solublty Correlatos of Carbo Doxde Polymers Cotag

More information

Centroids & Moments of Inertia of Beam Sections

Centroids & Moments of Inertia of Beam Sections RCH 614 Note Set 8 S017ab Cetrods & Momets of erta of Beam Sectos Notato: b C d d d Fz h c Jo L O Q Q = ame for area = ame for a (base) wdth = desgato for chael secto = ame for cetrod = calculus smbol

More information

A Study on the Mode Shape Piezoelectric Motor

A Study on the Mode Shape Piezoelectric Motor Ope Joural of Acoustcs, 015, 5, 5-65 Publshe Ole Jue 015 ScRes. http://www.scrp.org/joural/oja http://x.o.org/10.36/oja.015.5005 A Stuy o the Moe Shape Pezoelectrc Motor Jwo Mg Jou Departmet of Mechacal

More information

Non-degenerate Perturbation Theory

Non-degenerate Perturbation Theory No-degeerate Perturbato Theory Proble : H E ca't solve exactly. But wth H H H' H" L H E Uperturbed egevalue proble. Ca solve exactly. E Therefore, kow ad. H ' H" called perturbatos Copyrght Mchael D. Fayer,

More information

A Method for Damping Estimation Based On Least Square Fit

A Method for Damping Estimation Based On Least Square Fit Amerca Joural of Egeerg Research (AJER) 5 Amerca Joural of Egeerg Research (AJER) e-issn: 3-847 p-issn : 3-936 Volume-4, Issue-7, pp-5-9 www.ajer.org Research Paper Ope Access A Method for Dampg Estmato

More information

Experimental Fact: E = nhf

Experimental Fact: E = nhf CHAPTR 3 The xperimetal Basis of Quatum PHYS-3301 Lecture 4 Sep. 6, 2018 3.1 Discovery of the X Ray ad the lectro 3.2 Determiatio of lectro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio

More information

MHD motion in field-reversed configuration plasma

MHD motion in field-reversed configuration plasma J. Plasma Fuso Res. SERIES, Vol. 8 (9) MHD moto feld-reversed cofgurato plasma Taeko IKEYAMA, Masaor HIROI ad Yasuyuk NOGI College of Scece ad Techology, Nho Uversty, Tokyo, Japa (Receved: 1 September

More information

ENGI 4421 Propagation of Error Page 8-01

ENGI 4421 Propagation of Error Page 8-01 ENGI 441 Propagato of Error Page 8-01 Propagato of Error [Navd Chapter 3; ot Devore] Ay realstc measuremet procedure cotas error. Ay calculatos based o that measuremet wll therefore also cota a error.

More information

L5 Polynomial / Spline Curves

L5 Polynomial / Spline Curves L5 Polyomal / Sple Curves Cotets Coc sectos Polyomal Curves Hermte Curves Bezer Curves B-Sples No-Uform Ratoal B-Sples (NURBS) Mapulato ad Represetato of Curves Types of Curve Equatos Implct: Descrbe a

More information

5.1 Finite Difference Time Domain Technique (FDTD)

5.1 Finite Difference Time Domain Technique (FDTD) Cotets 5.1 Fte Dfferece Tme Doma Techque (FDTD) 5. Theoretcal aalss of cross patch atea 5.3 Theoretcal aalss of cross patch atea wth X-slot 5.4 Theoretcal aalss of Frequec recofgurable polarato dverst

More information

Computational Methods for Wave Based Sensing

Computational Methods for Wave Based Sensing Computatoal Methods for Wave Based Sesg Care M. Rappaport CeSSIS Dept. lect. ad Comp. geerg Northeaster Uverst IGRT Roudtable September 009 Care Rappaport 009 Wave-Based Modelg Fte Dfferece Tme Doma (FDTD)

More information

Theoretical background and applications of DEM. Simon Lo

Theoretical background and applications of DEM. Simon Lo Theoretcal backgroud ad applcatos of DEM Smo Lo Cotets DEM equatos DEM teracto models Examples Partcle trasport horzotal ppes Blast furace Mxg drum Coveyer belt cases Partcle trasport gas-lqud flow ppes

More information

Analyzing Control Structures

Analyzing Control Structures Aalyzg Cotrol Strutures sequeg P, P : two fragmets of a algo. t, t : the tme they tae the tme requred to ompute P ;P s t t Θmaxt,t For loops for to m do P t: the tme requred to ompute P total tme requred

More information

CLASS NOTES. for. PBAF 528: Quantitative Methods II SPRING Instructor: Jean Swanson. Daniel J. Evans School of Public Affairs

CLASS NOTES. for. PBAF 528: Quantitative Methods II SPRING Instructor: Jean Swanson. Daniel J. Evans School of Public Affairs CLASS NOTES for PBAF 58: Quattatve Methods II SPRING 005 Istructor: Jea Swaso Dael J. Evas School of Publc Affars Uversty of Washgto Ackowledgemet: The structor wshes to thak Rachel Klet, Assstat Professor,

More information

ECE606: Solid State Devices Lecture 13 Solutions of the Continuity Eqs. Analytical & Numerical

ECE606: Solid State Devices Lecture 13 Solutions of the Continuity Eqs. Analytical & Numerical ECE66: Sold State Devces Lecture 13 Solutos of the Cotuty Eqs. Aalytcal & Numercal Gerhard Klmeck gekco@purdue.edu Outle Aalytcal Solutos to the Cotuty Equatos 1) Example problems ) Summary Numercal Solutos

More information

UNIVERSITY OF OSLO DEPARTMENT OF ECONOMICS

UNIVERSITY OF OSLO DEPARTMENT OF ECONOMICS UNIVERSITY OF OSLO DEPARTMENT OF ECONOMICS Postpoed exam: ECON430 Statstcs Date of exam: Jauary 0, 0 Tme for exam: 09:00 a.m. :00 oo The problem set covers 5 pages Resources allowed: All wrtte ad prted

More information

Lesson 3. Group and individual indexes. Design and Data Analysis in Psychology I English group (A) School of Psychology Dpt. Experimental Psychology

Lesson 3. Group and individual indexes. Design and Data Analysis in Psychology I English group (A) School of Psychology Dpt. Experimental Psychology 17/03/015 School of Psychology Dpt. Expermetal Psychology Desg ad Data Aalyss Psychology I Eglsh group (A) Salvador Chacó Moscoso Susaa Saduvete Chaves Mlagrosa Sáchez Martí Lesso 3 Group ad dvdual dexes

More information

FREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM

FREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM Joural of Appled Matematcs ad Computatoal Mecacs 04, 3(4), 7-34 FREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM Ata Cekot, Stasław Kukla Isttute of Matematcs, Czestocowa Uversty of Tecology Częstocowa,

More information

Lecture 7. Confidence Intervals and Hypothesis Tests in the Simple CLR Model

Lecture 7. Confidence Intervals and Hypothesis Tests in the Simple CLR Model Lecture 7. Cofdece Itervals ad Hypothess Tests the Smple CLR Model I lecture 6 we troduced the Classcal Lear Regresso (CLR) model that s the radom expermet of whch the data Y,,, K, are the outcomes. The

More information

Mass Transport. Laboratory 3

Mass Transport. Laboratory 3 Laboratory 3 HWR 431/531 3-1 Itroducto: I the prevous laboratory we derved a expresso descrbg the flow of groudwater through a porous medum kow as Darcy's Law: Q = dh KA dl where Q = volumetrc dscharge

More information

Chapter 2 - Free Vibration of Multi-Degree-of-Freedom Systems - II

Chapter 2 - Free Vibration of Multi-Degree-of-Freedom Systems - II CEE49b Chapter - Free Vbrato of Mult-Degree-of-Freedom Systems - II We ca obta a approxmate soluto to the fudametal atural frequecy through a approxmate formula developed usg eergy prcples by Lord Raylegh

More information

Transforms that are commonly used are separable

Transforms that are commonly used are separable Trasforms s Trasforms that are commoly used are separable Eamples: Two-dmesoal DFT DCT DST adamard We ca the use -D trasforms computg the D separable trasforms: Take -D trasform of the rows > rows ( )

More information

ENGI 3423 Simple Linear Regression Page 12-01

ENGI 3423 Simple Linear Regression Page 12-01 ENGI 343 mple Lear Regresso Page - mple Lear Regresso ometmes a expermet s set up where the expermeter has cotrol over the values of oe or more varables X ad measures the resultg values of aother varable

More information

Analysis of Variance with Weibull Data

Analysis of Variance with Weibull Data Aalyss of Varace wth Webull Data Lahaa Watthaacheewaul Abstract I statstcal data aalyss by aalyss of varace, the usual basc assumptos are that the model s addtve ad the errors are radomly, depedetly, ad

More information

DISPLACEMENT-BASED SEISMIC DESIGN OF MDOF CONTINUOUS GIRDER BRIDGES

DISPLACEMENT-BASED SEISMIC DESIGN OF MDOF CONTINUOUS GIRDER BRIDGES 3 th World Coferece o Earthquake Egeerg Vacouver, B.C., Caada August -6, 004 Paper No. 05 DISPLACEMENT-BASED SEISMIC DESIGN OF MDOF CONTINUOUS GIRDER BRIDGES X ZHU ad Jawe HUANG SUMMARY The proposed procedure

More information

Progress In Electromagnetics Research C, Vol. 26, , 2012

Progress In Electromagnetics Research C, Vol. 26, , 2012 Progress I Electromagetcs Research C, Vol 6, 67 79, 0 THE CLOSE-FORM SOLUTION FOR SYMMETRIC BUTLER MATRICES C Leclerc,, *, H Aubert,, A Al,, A Aab 3, ad M Romer 4 CNRS; LAAS; 7 Aveue Du Coloel Roche, Toulouse

More information

hp calculators HP 30S Statistics Averages and Standard Deviations Average and Standard Deviation Practice Finding Averages and Standard Deviations

hp calculators HP 30S Statistics Averages and Standard Deviations Average and Standard Deviation Practice Finding Averages and Standard Deviations HP 30S Statstcs Averages ad Stadard Devatos Average ad Stadard Devato Practce Fdg Averages ad Stadard Devatos HP 30S Statstcs Averages ad Stadard Devatos Average ad stadard devato The HP 30S provdes several

More information

Lecture Notes Types of economic variables

Lecture Notes Types of economic variables Lecture Notes 3 1. Types of ecoomc varables () Cotuous varable takes o a cotuum the sample space, such as all pots o a le or all real umbers Example: GDP, Polluto cocetrato, etc. () Dscrete varables fte

More information

The complex Jacobi iterative method for threedimensional wide-angle beam propagation

The complex Jacobi iterative method for threedimensional wide-angle beam propagation The complex Jacob teratve method for threedmesoal wde-agle beam propagato Kha Q. Le R. Godoy-Rubo eter Bestma ad G. Roald Hadley 3 Departmet of Iformato Techology Ghet Uversty-IMEC St- eterseuwstraat 4

More information

Computational Geometry

Computational Geometry Problem efto omputatoal eometry hapter 6 Pot Locato Preprocess a plaar map S. ve a query pot p, report the face of S cotag p. oal: O()-sze data structure that eables O(log ) query tme. pplcato: Whch state

More information

d b c d a c a a a c d b

d b c d a c a a a c d b Beha Uverty Faculty of Egeerg Shoubra Electrcal Egeerg eartmet Frt Year commucato. t emeter Eam ate: 3 0 ECE: Electroc Egeerg fudametal urato : 3 hour K=.38 3 J/K h=6.64 34 J. q=.6 9 C m o =9. 3 Kg [S]

More information

Wu-Hausman Test: But if X and ε are independent, βˆ. ECON 324 Page 1

Wu-Hausman Test: But if X and ε are independent, βˆ. ECON 324 Page 1 Wu-Hausma Test: Detectg Falure of E( ε X ) Caot drectly test ths assumpto because lack ubased estmator of ε ad the OLS resduals wll be orthogoal to X, by costructo as ca be see from the momet codto X'

More information

15. Nanoparticle Optics in the Electrostatic Limit

15. Nanoparticle Optics in the Electrostatic Limit 5 aopartcle Optcs the lectrostatc Lmt I the prevous chapter, we were restrcted to aospheres because a full soluto of Maxwell s equato was eeded Such a aalytc calculato s oly possble for very smple geometres

More information

Median as a Weighted Arithmetic Mean of All Sample Observations

Median as a Weighted Arithmetic Mean of All Sample Observations Meda as a Weghted Arthmetc Mea of All Sample Observatos SK Mshra Dept. of Ecoomcs NEHU, Shllog (Ida). Itroducto: Iumerably may textbooks Statstcs explctly meto that oe of the weakesses (or propertes) of

More information

Simulation Output Analysis

Simulation Output Analysis Smulato Output Aalyss Summary Examples Parameter Estmato Sample Mea ad Varace Pot ad Iterval Estmato ermatg ad o-ermatg Smulato Mea Square Errors Example: Sgle Server Queueg System x(t) S 4 S 4 S 3 S 5

More information

d dt d d dt dt Also recall that by Taylor series, / 2 (enables use of sin instead of cos-see p.27 of A&F) dsin

d dt d d dt dt Also recall that by Taylor series, / 2 (enables use of sin instead of cos-see p.27 of A&F) dsin Learzato of the Swg Equato We wll cover sectos.5.-.6 ad begg of Secto 3.3 these otes. 1. Sgle mache-fte bus case Cosder a sgle mache coected to a fte bus, as show Fg. 1 below. E y1 V=1./_ Fg. 1 The admttace

More information