Wisconsin Milwaukee - LING - 320

LING3201 First Language Acquisition Term Project paper 2011Natalie Yu Tsz Sum (1155000186) FallUsage and Development of Cantonese Sentence-final Particles wo3, wo4, and wo5 in native Cantonese-speaking Children1. Introduction Sentence-final ParticlesS

University of Illinois, Urbana Champaign - MSE - 461

MatSE 361 OUTLINE I. INTRODUCTION Syllabus Overview Introduction - Scales Introduction - Devices Introduction - Processes Introduction - Pressure: Molecules in VacuumLatest FILENAME: MatSE 461 Chapter 1 Intro Syllabus Scales Device Process w outline 8-28

University of Illinois, Urbana Champaign - MSE - 461

MatSE 361 OUTLINE: 2. Si Substrate Preparation OUTLINE 2. Si Substrate Preparation Overall Process Wafer production Impurities in as Grown Si Denuding Process: Process Flow Denuding Process: Diffusion Review (Ch. 7 Mayer) Denuding Process: Quantitative SO

University of Illinois, Urbana Champaign - MSE - 461

MatSE 361 OUTLINE: 3. Ion Implantation OUTLINE 3. Ion Implantation Introduction Machine Simulation Energy Loss Mechanisms Ion-Nucleus Interaction SOI: Hydrogen in Si RBS and Channeling1MatSE 361 Chapter 0 Syllabus, IntroMatSE 361 OUTLINE: 3. Ion Implan

University of Illinois, Urbana Champaign - MSE - 461

MatSE 361 4- R-C-Size Material NOTES Old Chapter B: Resistance and Capacitance1MatSE 361 Chapter B Resistance and CapacitanceOUTLINE2MatSE 361 Chapter B Resistance and CapacitanceIntroduction: Current Flow and CapacitanceCurrent flow from point A t

University of Illinois, Urbana Champaign - MSE - 461

MatSE 361 OUTLINE: 5. MOS Capacitor Outline 5. MOS Capacitor Band DiagramIdeal metal-dielectric-semiconductor configuration Charge Distribution at difference bias voltagesApplications Electrostatics Hi-k Dielectrics Electrical Characterization of MOS Ca

University of Illinois, Urbana Champaign - MSE - 461

MatSE 361 OUTLINE: 6. MOSFET OUTLINE 6. MOSFET INTRO - Connection to MOS Capacitor MOSFET Ideal MOSFET/MOS Non-ideal MOSFET Fabrication1MatSE 361 Chapter 0 Syllabus, IntroMatSE 361 OUTLINE: 6. MOSFET Intro 6. MOSFET INTRO - Connection to MOS Capacitor

University of Illinois, Urbana Champaign - MSE - 461

ARTICLESPUBLISHED ONLINE: 10 JULY 2011 | DOI: 10.1038/NMAT3070A fast, high-endurance and scalable non-volatile memory device made from asymmetric Ta2O5-x/TaO2-x bilayer structuresMyoung-Jae Lee1 *, Chang Bum Lee1 , Dongsoo Lee1 , Seung Ryul Lee1 , Man

University of Illinois, Urbana Champaign - MSE - 461

A fast, high-endurance and scalable nonvolatile memory device made from asymmetric Ta2O5-x / TaO2-x bilayer structuresMyoung-Jae Lee, Chang Bum Lee, Dongsoo Lee, Seung Ryul Lee, Man Chang, Ji Hyun Hur Young-Bae Kim, Chang-Jung Kim, David H. Seo, Sunae Se

University of Illinois, Urbana Champaign - MSE - 461

ARTICLESPUBLISHED ONLINE: 25 JANUARY 2009 DOI: 10.1038/NMAT2373Conduction at domain walls in oxide multiferroicsJ. Seidel1,2 * , L. W. Martin2,3 *, Q. He1 , Q. Zhan2 , Y.-H. Chu2,3,4 , A. Rother5 , M. E. Hawkridge2 , P. Maksymovych6 , P. Yu1 , M. Gajek

University of Illinois, Urbana Champaign - MSE - 461

CONDUCTION AT DOMAIN WALLS IN OXIDE MULTIFERROICSBy J. Seidel, et al. MSE 461Presented by Amber Choquette Date: September 23rd, 2011ABSTRACTDomain walls may play an important role in future electronic devices, given their small size as well as the fac

University of Illinois, Urbana Champaign - MSE - 461

Low-Power Switching of Phase-Change Materials with Carbon Nanotube Electrodes Feng Xiong, et al. Science 332, 568 (2011); DOI: 10.1126/science.1201938This copy is for your personal, non-commercial use only.If you wish to distribute this article to other

University of Illinois, Urbana Champaign - MSE - 461

Low-Power Switching of Phase-Change Materials with Carbon Nanotube ElectrodesFeng Xiong, Albert D. Liao, David Estrada, Eric PopMatSE 461 Jongmin Youn 30 September 2011F. Xiong, A.D. Liao, D. Estrada, E. Pop, "Low Power Switching of Phase-Change Materi

University of Illinois, Urbana Champaign - MSE - 461

Surface Crystallization in a Liquid AuSi Alloy Oleg G. Shpyrko, et al. Science 313, 77 (2006); DOI: 10.1126/science.1128314This copy is for your personal, non-commercial use only.If you wish to distribute this article to others, you can order high-quali

University of Illinois, Urbana Champaign - MSE - 461

Science Vol. 313 7 JULY 2006Surface Crystallization in a Liquid AuSi AlloyBy Oleg G. Shpyrko et al., Harvard- A Literature Study -For MatSE 461 -By Zichao Sept. 2nd 1Content Abstract (3) Introduction (47) Methods (8) Results (916) Problem Discussio

University of Illinois, Urbana Champaign - MSE - 461

ARTICLELaser-Synthesized Epitaxial GrapheneSangwon Lee, Michael F. Toney, Wonhee Ko, Jason C. Randel, Hee Joon Jung, Ko Munakata, Jesse Lu, Theodore H. Geballe, Malcolm R. Beasley, Robert Sinclair, Hari C. Manoharan, ,# and Alberto Salleo,* Department o

University of Illinois, Urbana Champaign - MSE - 461

LaserSynthesized Epitaxial GraphenePublished in: Sangwon Lee; Michael F. Toney; Wonhee Ko; Jason C. Randel; Hee Joon Jung; Ko Munakata; Jesse Lu; Theodore H. Geballe; Malcolm R. Beasley; Robert Sinclair; Hari C. Manoharan; Alberto Salleo; ACS Nano 2010,

University of Illinois, Urbana Champaign - MSE - 461

www.advmat.de www.MaterialsViews.comCOMMUNICATIONPolarizing Organic PhotovoltaicsRui Zhu, Ankit Kumar, and Yang Yang*Today's most prevalent information display technology is the liquid crystal display (LCD). Unfortunately, LCDs are energy inefficient,

University of Illinois, Urbana Champaign - MSE - 461

Polarizing Organic Photovoltaics08/09/2011Advanced MaterialsRui Zhu , Ankit Kumar , and Yang YangYou Zhai (Andy) MSE 46109/16/2011MSE 461 1OutlineI. II. III. IV. V. Background Strategy Methods & Results Summary & Outlook ReferencesMSE 461 2Backg

University of Illinois, Urbana Champaign - MSE - 461

Published on Web 05/11/2010Nanoscale Structure, Composition, and Charge Transport Analysis of Transparent Conducting Oxide Nanowires Written by Focused Ion Beam ImplantationNorma E. Sosa, Christopher Chen, Jun Liu, Sujing Xie, Tobin J. Marks,*, and Mark

University of Illinois, Urbana Champaign - MSE - 461

Analysis of Transparent Conducting Oxide Nanowires Publication by: N. E. Sosa, et. Al. Presentation by: Chad 1All transparent circuitryApplications/Motivation for TCOsSemiconductors, conductors and insulatorsPaper focuses on Transparent Conducting Oxi

University of Illinois, Urbana Champaign - MSE - 461

LETTERSTailoring the atomic structure of graphene nanoribbons by scanning tunnelling microscope lithography LEVENTE TAPASZTO1*, GERGELY DOBRIK1, PHILIPPE LAMBIN2 AND LASZLO P. BIRO11 2Research Institute for Technical Physics and Materials Science, H-1

University of Illinois, Urbana Champaign - MSE - 461

Tailo ring the Ato mic S truc ture o f Graphe ne Nano ribbo ns by S c anning Tunne ling Mic ro s c o pe Litho g raphy 1 Authors: Levente Tapaszto, Gergely Dobrik, Phillipe Lambin, Laszlo P Biro MatSe461 Adrian Radocea 1.Tapaszto, L. et al. (2008). Tailor

University of Illinois, Urbana Champaign - MSE - 461

Tailo ring the Ato mic S truc ture o f Graphe ne Nano ribbo ns by S c anning Tunne ling Mic ro s c o pe Litho g raphy Adrian RadoceaAuthors: Levente Tapaszto, Gergely Dobrik, Phillipe Lambin, Laszlo P Biro MatSe461 Adrian Radocea Nov 14th, 20111Tailo r

University of Illinois, Urbana Champaign - MSE - 461

Chapter K : Photolithography in MicroelectronicsIntroduction How does it work? Properties of PR Techniques Liftoff: image reversal Types of Lithography Image vs Direct write Physics Optics Phase Shift masks Future Limits Chemistry Acids, bases, solubilit

University of Illinois, Urbana Champaign - MSE - 461

MatSE 361 OUTLINE: 2. Si Substrate Preparation OUTLINE 2. Si Substrate Preparation Overall Process Wafer production Impurities in as Grown Si Denuding Process: Process Flow Denuding Process: Diffusion Review (Ch. 7 Mayer) Denuding Process: Quantitative SO

University of Illinois, Urbana Champaign - MSE - 461

MatSE 361 OUTLINE: 3. Ion Implantation OUTLINE 3. Ion Implantation Introduction Machine Simulation Energy Loss Mechanisms Ion-Nucleus Interaction SOI: Hydrogen in Si RBS and Channeling1MatSE 361 Chapter 0 Syllabus, IntroMatSE 361 OUTLINE: 3. Ion Implan

University of Illinois, Urbana Champaign - MSE - 461

MatSE 361 OUTLINE I. INTRODUCTION Syllabus Overview Introduction - Scales Introduction - Devices Introduction - Processes Introduction - Pressure: Molecules in VacuumLatest FILENAME: MatSE 461 Chapter 1 Intro Syllabus Scales Device Process w outline 8-28

University of Illinois, Urbana Champaign - PHYS - 560

Overview Solid = collection of atoms (~1023, a huge number) Crystalline: single crystals, polycrystalline materials Amorphous, glassy materials Others: liquid crystals, quasicrystals, partially ordered polymers, . Theory of solids to explain and predict p

University of Illinois, Urbana Champaign - PHYS - 560

Sommerfeld Theory of Metals a quantum theory of independent free electrons Physical picture: Focus on one electron. Assume all other charges in the system are smeared out into a static neutral background (atomic details, fluctuations, & correlations ignor

University of Illinois, Urbana Champaign - PHYS - 560

Review Drude model (free electron approximation) + (independent electron approximation) + (Maxwell Boltzmann statistics) Sommerfeld model (free electron approximation) + (independent electron approximation) + (Fermi Dirac statistics) Next: Band structure

University of Illinois, Urbana Champaign - PHYS - 560

Reciprocal Lattice Direct lattice given by R ni aiiDefinition: reciprocal lattice is a Bravais lattice given byK = reciprocal lattice vectors i bi , where i = integers, anda2 a3 a 3 a1 a1 a 2 b1 2 ; b2 2 ; b3 2 a1 a 2 a 3 a1 a 2 a 3 a1 a 2 a 3Useful

University of Illinois, Urbana Champaign - PHYS - 560

X-Ray Diffraction A method to determine crystal structure. Assumption: ignoring thermal vibrations of lattice (including zero-point vibrations) for now. A charged particle of charge q in an EM field:1 q H p A V r 2m c 2 1 2 q q q2 p A p p A 2 A2 V r 2m

University of Illinois, Urbana Champaign - PHYS - 560

Electronic States in a Crystal ~1023 interacting electrons and ion cores a big computational problem. p2 1 p2 Z Z e2 1 e2 n n n HT i i 2m 2 i , j ri r j n 2Mn 2 n,n ' R n R n Hspin-orbit-interaction . Hel H core H el core Hsoi . Z e2 n n,i ri R n Frozen

University of Illinois, Urbana Champaign - PHYS - 560

Band Structure Calculations using a plane wave basis set 2 2 k r U r k r k k r 2mFourier transform: U r UK e iK rK k r e ik r uk r e ik r ck-K e iK r e ik r ck+K e iK rK K2 2m c k K k-K K2ei k K r UK e iK r ck-K e K Ki k K r kcKk-Kei k

University of Illinois, Urbana Champaign - PHYS - 560

Density of States: g Definition: g d = number of states between and d (per unit volume) For a single band k , g d 1 V1 8 d3 k ,s dd23k1 4 3 dS dkddk dS = area element on constant energy surface k dk = change in k, along k k (perpendicular to d

University of Illinois, Urbana Champaign - PHYS - 560

Screening (Electron-Electron Interaction) Classical pictureEextClassical metal Ein 0The internal field is zero. Electrons are free to move; a layer of charge (screening charge) accumulates at the surface. The external field is screened. Quantum picture

University of Illinois, Urbana Champaign - PHYS - 560

Electron Dynamics (of Semiconductors) Basic assumption: independent electron approximation (single-particle picture) Question: what happens to an electron under an external field (transport properties)? Bloch state nk e ik r uk r p nk i nk e ik r p k uk

University of Illinois, Urbana Champaign - PHYS - 560

Lattice Waves Thus far, static lattice model. In reality, atoms vibrate even at T 0 because of zero-point vibration. Monatomic Crystals Basis = 1 atom.r R R u R;t Lattice: R ni aiii 1,2,3Actual atomic position = lattice position + vibrationu 0rave

University of Illinois, Urbana Champaign - PHYS - 560

Lattice Specific Heat Classical: Equi-partition theorem:1 1 1 kx x2 mvx 2 kT 2 2 26 degrees of freedom each atom 3 each from kinetic energy and potential energy. Internal energy/volume u Volume specific heat CV 33NkT ; N = total number of atoms (includ

University of Illinois, Urbana Champaign - PHYS - 560

Anharmonic Effects Assume one atom per unit cell. Potential energy U r R UR u R U U 0 harmonic potential u 2 O u 3 O u 4 Terms O u 3 , O u 4 anharmonic effects or phonon-phonon interactions uR 1 Nks2 M s (k )aks + a-ks e s (k )eik RO u 3 . a a a

University of Illinois, Urbana Champaign - PHYS - 560

Neutron Scattering Counts E E' E Spectrum at a fixed scattering geometry: elastic peak caused by defect scattering (or Bragg diffraction) one-phonon emission peaks at lower energies (Stokes peaks) one-phonon absorption peaks at higher energies (anti-Stoke

University of Illinois, Urbana Champaign - PHYS - 560

Infrared Properties (of Ionic Crystals) Assume the system is nonmagnetic, 1 . Optical properties determined by the dielectric function, D E. Assume cubic symmetry. D E Assume no free charges. D 0 DEP ik E 0 E ik E 4 ( = bound charge density) Longitudinal

University of Illinois, Urbana Champaign - PHYS - 560

Magnetism B H 4 M H M = magnetizationBi Bo Bournday conditions: B 0 4 1 D H j 0 , assuming steady state and no free current c c tH i H oFerromagnetic Paramagnetic DiamagneticM 0 for B a 0 (zero applied field); generally nonlinear BH ~ constant ~ 1 + O

University of Illinois, Urbana Champaign - PHYS - 560

Ferromagnetism A simple picture: ferromagnetism arises from "atomic magnets" aligned in the same direction. What is the interaction to align them? Each atomic magnetic has a magnetic moment ~ g0 B . Dipolar interaction energy between neighboring atomic ma

University of Illinois, Urbana Champaign - PHYS - 560

Crystallographic restriction theorem See: http:/en.wikipedia.org/wiki/Crystallographic_restriction_theorem Problem: Consider rotational symmetry operations of a 2D periodic lattice with the rotation axis perpendicular to the lattice plane. Show that only

University of Illinois, Urbana Champaign - PHYS - 560

Physics 560 Homework problem set 1 1. A&M Problem 1, Chapter 1. 2. A&M Problem 2, Chapter 1. 3. A&M Problem 3, Chapter 1. 4. Recall 1 i 4 , where is the conductivity derived from the valence electrons.This expression was derived assuming that the posit

Rutgers - FINANCE - 250

March 27, 2012 Leasing versus buying a car You build no equity You are still responsible for maintenance and damages You are charged extra for o Too many miles (over 12,000 miles) o Ending the lease early will charge a penalty Buying a car . would you tak

Rutgers - FINANCE - 250

Government Health Care Plans Medicare Provides health insurance to people over age 65 Part A covers inpatient care in hospitals or nursing facilities and some home health Part B is optional coverage Part C is a combination of Part A and Part B provide

Rutgers - FINANCE - 250

Chapter 12: Health and Disability Insurance Health Insurance Health insurance: a type of insurance offered by private insurance companies or the government that covers health care expenses incurred by policyholders for necessary medical care Critical comp

University of Texas - PHY - 102M

Question 14 out of 4 pointsRead the derivation for acceleration of the 2 objects in Atwood machine system in your manual. If we have m1=150g, m2=155g, what's the acceleration (m1 goes up and m2 goes down)? Answer Selected Answer: 0.161m/(s^2)Question

University of Texas - PHY - 102M

Question 13 out of 3 pointsLook at Fig. 4-1 in your manual, let's say PEtot is the total potential energy of masses m1 and m2 (m1<m2). After m1 goes up by a distance d, and m2 goes down the same distance. The change in PEtot is (when something goes up

University of Texas - PHY - 102M

Question 13 out of 3 pointsPick the right descriptions for inelastic collision Answer Selected Answers:Question 23 out of 3 pointsPick the right descriptions for completely elastic collision Answer Selected Answers:Question 33 out of 3 pointsIf m

University of Texas - PHY - 102M

Question 13 out of 3 pointsWhen considering rotational motion there are similarities between rotational motion and translational motion. Look at the table, answer question 1&2 Translational D (displacement) V (velocity) A (acceleration) F (force) P (mo

University of Texas - PHY - 102M

Question 13 out of 3 pointsWhat are the necessary conditions for objects in translational and rotational equilibrium? is torque on the object(s), F is the force on the object(s), v is the translational velocity of the object(s), and is the angular velo

University of Texas - PHY - 102M

Question 13 out of 3 pointsOn graph paper draw a vector from the origin of a graph 8 cm at 0 degrees from the x-axis. Now add a vector at 90 degrees and 6 cm long to the first vector. What is the length of the addition calculated? What is the direction

Columbia State Community College - FREN - 1200

MBG*2040 Foundations in Molecular Biology and GeneticsMock Midterm Exam Winter 2012 It is most beneficial to you to write this mock midterm UNDER EXAM CONDITIONS. This means: Complete the midterm in an hour and 15 minutes. Work on your own. Keep your not

Columbia State Community College - FREN - 1200

STAT*2040 TERM TEST II PRACTICE PACKAGEWinter 2012DISCLAIMERThis resource is not designed to be used independently of the SLG Session listed above. Please use this resource for referral only it is supplemental review and is not meant to be a substitute

Columbia State Community College - FREN - 1200

University of Ottawa - BIO - 3170

Bio 1540 ; questions de rvision : signalisation cellulaire8.1 Communication cellulaire1- Quelles sont les tapes de la signalisation cellulaire ? 1. rception 2.transduction 3. rponse 2- Quand est-ce que des molcules sont scrtes pour envoyer un message ce

University of Ottawa - BIO - 3170

Bio 1540 ; questions de rvision : signalisation cellulaire8.2 Rception cellulaire1- Classez en ordre en numrotant les tapes de la rception cellulaire : Entre des molcules (ex: ions) dans la cellule 4 Massager primaire circulant ou membranaire 1Changeme