Solutions for Assignment-8

Size: px
Start display at page:

Download "Solutions for Assignment-8"

Transcription

1 Solutions for Assignment-8 Q1. The process of adding impurities to a pure semiconductor is called: [1] (a) Mixing (b) Doping (c) Diffusing (d) None of the above In semiconductor production, doping intentionally introduces impurities into an extremely pure intrinsic semiconductor for the purpose of modulating its electrical properties. Q2. The pentavalent impurities; i.e., antimony, arsenic, bismuth, phosphorus, etc., added to intrinsic semiconductors are called: [1] (a) Acceptor or P-type impurities (b) Donor or P-type impurities (c) Acceptor or N-type impurities (d) Donor or N-type impurities The number of electrons in pentavalent impurities i.e. antimony, arsenic, bismuth, and phosphorus are higher than the number of holes due to which they are considered as a donor or N-type impurities. Q3. The functionalization of nanomaterials is carried out through: [1] (a) Adsorption of functional groups (b) Attachment of functional groups (c) Absorption of functional groups (d) None of these Functionalization of nanomaterials includes the possibility of attaching functional groups to the nanomaterials (such as fullerene, carbon nanodots, CNTs, graphene, etc.) surface with molecular moieties possessing suitable properties that are essential for the realization of new molecular hybrid materials with novel/enhanced functions.

2 Q4. Which of the following properties can be improved through functionalization of a nanomaterial? [1] (a) Thermal stability (b) Dispersibility (c) Interfacial bonding (d) All of the above Different chemical and physical functionalizations of nanomaterials are found be effective for improving the thermal stability, electrical conductivity, processibility, dispersibility, interfacial properties and various mechanical, barrier and sensing properties. Q5. What is the effect of temperature on physical adsorption? [1] (a) Increases with increase in temperature (b) Increases with decrease in temperature (c) Decreases with increase in temperature (d) No effect Since physical adsorption is an exothermic process, it occurs more readily at lower temperatures and decreases with increase in temperature (Le-Chatelier's Principle). Q6. Which of the following bonds should be present in organosilanes? [1] (a) Si-O (b) Si-C (c) Si-Cl (d) Si-H Organosilanes consist of silane with at least one Si-C bond. Q7. Defect functionalization includes: [1] (a) Esterification (b) Fluorination (c) Hydrogenation (d) Cycloaddition

3 Defect functionalization includes amidation, esterification, thiolation, silanization and polymer grafting. Q8. Which of the following characterization techniques help to prominently identify the presence of functional groups? [1] (i) XPS; (ii) XRD; (iii) EDAX; (iv) FTIR (a) (ii) and (iv) (b) (ii) and (iii) (c) (i) and (iv) (d) (iii) and (iv) XPS and FTIR are most widely used to observe the presence of specific functional groups on the surface of a nanomaterial. Q9. Which of the following methods can be used to enable grafting on a particle through modifying the polymer end-chain after polymerization? [1] (a) Grafted from (b) Grafted onto (c) Both of these (d) None of these In grafted onto method, polymer end-chain can be modified after polymerization to enable grafting on the particle. Q10. Stöber method was originally designed for: [1] (a) Titania nanoparticles (b) Zirconia nanoparticles (c) Silica nanoparticles (d) Alumina nanoparticles Silica has been widely used since the invention of the Stöber method which was originally designed for the preparation of silica nanoparticles with well controlled spherical shape and size using alcoholic solvents, catalysts and alkoxide precursors. Q11. In an intrinsic semiconductor, the position of Fermi level lies: [2]

4 (a) At the center of forbidden energy gap (b) Near the conduction band (c) Near the valence band (d) Anywhere in the forbidden energy gap The Fermi level for n-type semiconductors is below the conduction band, for p-type semiconductors, it is above the valence band and for intrinsic (pure) semiconductors it is exactly at the center of forbidden energy gap. Q12. Choose a suitable option which provides correct explanations (Section B) for the surface modification methods (Section A): [2] Section A Section B 1. Doping (i) Gas molecules condense on the surface 2. Adsorption (ii) Attaching functional groups 3. Grafting (iii) Adding impurities or replacing host atoms 4. Functionalization (iv) Addition of polymer chains onto a surface (a) 1-(ii), 2-(iv), 3-(i), 4-(iii) (b) 1-(ii), 2-(iii), 3-(iv), 4-(i) (c) 1-(iii), 2-(i), 3-(iv), 4-(ii) (d) 1-(ii), 2-(iv), 3-(i), 4-(iii) Doping is the process of adding some impurity atoms or replacing host atoms in the semiconductor.

5 Adsorption is the adhesion of atoms, ions, or molecules from a gas, liquid, or dissolved solid to a surface. This process creates a film of the adsorbate on the surface of the adsorbent. Grafting, in the context of polymer chemistry, refers to the addition of polymer chains onto a surface. Functionalization is the possibility of attaching functional groups to the nanomaterials (such as fullerene, carbon nanodots, CNTs, graphene, etc) surface with molecular moieties possessing suitable properties that are essential for the realization of new molecular hybrid materials with novel/enhanced functions. Q13. Which of the following conditions is not true for the doping of nitrogen in graphene? [2] (a) Atomic radius is almost same (b) Same crystal structure (c) Electro-positives are 2.55 for C and 3.04 for N (d) Valences are +3 for C and +3, +5 for N N-doped graphene, having following necessary conditions: Atomic radii of C and N are 70 pm and 65 pm, respectively Both have HCP crystal structure, Electro-negativities are 2.55 for C and 3.04 for N Valencies are +3 for C and +3, +5 for N Q14. Match the techniques given in Section A with their applications in Section B : [2] Section A Section B 1. Doping (i) Lenses 2. Functionalization (ii) Membranes for the separation of gases or liquids 3. Polymerization (PMMA) (iii) Molecular junctions, FETs 4. Grafting (iv) Photovoltaics, Supercapacitors (a) 1-(ii), 2-(iv), 3-(iii), 4-(i) (b) 1-(iv), 2-(i), 3-(iii), 4-(ii)

6 (c) 1-(iv), 2-(iii), 3-(i), 4-(ii) (d) 1-(ii), 2-(iii), 3-(iv), 4-(i) Doping: Electro catalysis, Li-ion battery (LIB) anodes, supercapacitors, sensing, photovoltaics, biological and biomedical applications. Functionalization: Molecular junctions, Field-effect transistors (FETs), solar thermal storage, memory devices, color sensing, biological applications. Polymerization (PMMA): Lenses, transparent aircraft enclosures, drafting equipment, outdoor signs, etc. Grafting: Membranes for the separation of gases or liquids, hydrogels, drug deliverers, thermoplastic elastomers, compatibilizers for polymer blends, polymeric emulsifiers, impact resistant plastics. Q15. Match the following techniques on the basis of their problems: [2] Techniques Problems 1. Coating (i) Agglomeration during wall formation 2. Microencapsulation (ii) Difficult to maintain the crystal structure of base material 3. Thin film (iii) Hiding functional characteristics of base material 4. Doping (iv) Damage during etching (a) 1-(ii), 2-(iv), 3-(iii), 4-(i) (b) 1-(iv), 2-(i), 3-(iii), 4-(ii) (c) 1-(iii), 2-(i), 3-(iv), 4-(ii) (d) 1-(ii), 2-(iii), 3-(iv), 4-(i) Problems during fabrication of thin film: Uniform film thickness, adhesion, cracks formation, damage thin film during etching or transfer one substrate to other, film deposition on reactor walls. Problems during microencapsulation:

7 A common problem in many microencapsulation processes is the agglomeration of capsules during wall formation. As the wall materials change from liquid to solid form they often go through a sticky stage which makes agglomeration difficult to avoid. Main problems in the coating of nanostructures: Uniformity of layer (thickness), surface roughness, agglomeration, corrosion prevention, hiding functional characteristics (optical, electrical and magnetic) of the substrate, optimal wettability, chemical composition (crystalline structure in nanometer range), standardize surface geometry. Problems during doping: It is very difficult to maintain the crystal structure of host material, during the doping process.

CLASS 12th. Semiconductors

CLASS 12th. Semiconductors CLASS 12th Semiconductors 01. Distinction Between Metals, Insulators and Semi-Conductors Metals are good conductors of electricity, insulators do not conduct electricity, while the semiconductors have

More information

e - Galvanic Cell 1. Voltage Sources 1.1 Polymer Electrolyte Membrane (PEM) Fuel Cell

e - Galvanic Cell 1. Voltage Sources 1.1 Polymer Electrolyte Membrane (PEM) Fuel Cell Galvanic cells convert different forms of energy (chemical fuel, sunlight, mechanical pressure, etc.) into electrical energy and heat. In this lecture, we are interested in some examples of galvanic cells.

More information

Lecture (02) Introduction to Electronics II, PN Junction and Diodes I

Lecture (02) Introduction to Electronics II, PN Junction and Diodes I Lecture (02) Introduction to Electronics II, PN Junction and Diodes I By: Dr. Ahmed ElShafee ١ Agenda Current in semiconductors/conductors N type, P type semiconductors N Type Semiconductor P Type Semiconductor

More information

Monolithic Cells for Solar Fuels

Monolithic Cells for Solar Fuels Electronic Supplementary Material (ESI) for Chemical Society Reviews. This journal is The Royal Society of Chemistry 2014 Monolithic Cells for Solar Fuels Jan Rongé, Tom Bosserez, David Martel, Carlo Nervi,

More information

Chapter 12 - Modern Materials

Chapter 12 - Modern Materials Chapter 12 - Modern Materials 12.1 Semiconductors Inorganic compounds that semiconduct tend to have chemical formulas related to Si and Ge valence electron count of four. Semiconductor conductivity can

More information

Lecture (02) PN Junctions and Diodes

Lecture (02) PN Junctions and Diodes Lecture (02) PN Junctions and Diodes By: Dr. Ahmed ElShafee ١ I Agenda N type, P type semiconductors N Type Semiconductor P Type Semiconductor PN junction Energy Diagrams of the PN Junction and Depletion

More information

Unit IV Semiconductors Engineering Physics

Unit IV Semiconductors Engineering Physics Introduction A semiconductor is a material that has a resistivity lies between that of a conductor and an insulator. The conductivity of a semiconductor material can be varied under an external electrical

More information

Basic Semiconductor Physics

Basic Semiconductor Physics 6 Basic Semiconductor Physics 6.1 Introduction With this chapter we start with the discussion of some important concepts from semiconductor physics, which are required to understand the operation of solar

More information

Lecture 1. OUTLINE Basic Semiconductor Physics. Reading: Chapter 2.1. Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations

Lecture 1. OUTLINE Basic Semiconductor Physics. Reading: Chapter 2.1. Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations Lecture 1 OUTLINE Basic Semiconductor Physics Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations Reading: Chapter 2.1 EE105 Fall 2007 Lecture 1, Slide 1 What is a Semiconductor? Low

More information

Ga and P Atoms to Covalent Solid GaP

Ga and P Atoms to Covalent Solid GaP Ga and P Atoms to Covalent Solid GaP Band Gaps in Binary Group III-V Semiconductors Mixed Semiconductors Affect of replacing some of the As with P in GaAs Band Gap (ev) (nm) GaAs 1.35 919 (IR) GaP 2.24

More information

Synthesis Breakout. Overarching Issues

Synthesis Breakout. Overarching Issues Synthesis Breakout. Overarching Issues 1. What are fundamental structural and electronic factors limiting Jsc, Voc, and FF in typical polymer bulk-heterojunction cells? Rational P- and N-type materials

More information

Nanotechnology and Solar Energy. Solar Electricity Photovoltaics. Fuel from the Sun Photosynthesis Biofuels Split Water Fuel Cells

Nanotechnology and Solar Energy. Solar Electricity Photovoltaics. Fuel from the Sun Photosynthesis Biofuels Split Water Fuel Cells Nanotechnology and Solar Energy Solar Electricity Photovoltaics Fuel from the Sun Photosynthesis Biofuels Split Water Fuel Cells Solar cell A photon from the Sun generates an electron-hole pair in a semiconductor.

More information

Introduction to Photolithography

Introduction to Photolithography http://www.ichaus.de/news/72 Introduction to Photolithography Photolithography The following slides present an outline of the process by which integrated circuits are made, of which photolithography is

More information

Self-study problems and questions Processing and Device Technology, FFF110/FYSD13

Self-study problems and questions Processing and Device Technology, FFF110/FYSD13 Self-study problems and questions Processing and Device Technology, FFF110/FYSD13 Version 2016_01 In addition to the problems discussed at the seminars and at the lectures, you can use this set of problems

More information

Atoms? All matters on earth made of atoms (made up of elements or combination of elements).

Atoms? All matters on earth made of atoms (made up of elements or combination of elements). Chapter 1 Atoms? All matters on earth made of atoms (made up of elements or combination of elements). Atomic Structure Atom is the smallest particle of an element that can exist in a stable or independent

More information

smal band gap Saturday, April 9, 2011

smal band gap Saturday, April 9, 2011 small band gap upper (conduction) band empty small gap valence band filled 2s 2p 2s 2p hybrid (s+p)band 2p no gap 2s (depend on the crystallographic orientation) extrinsic semiconductor semi-metal electron

More information

Report on Preparation of Nanotemplates for mab Crystallization

Report on Preparation of Nanotemplates for mab Crystallization Deliverable number D2.1 Due date 30/09/2017 Deliverable title Report on Preparation of Nanotemplates for mab Crystallization Issue date 21/09/2017 WP number WP2 Author(s) J. Heng, W. Chen, H. Yang Lead

More information

Nanostrukturphysik (Nanostructure Physics)

Nanostrukturphysik (Nanostructure Physics) Nanostrukturphysik (Nanostructure Physics) Prof. Yong Lei & Dr. Yang Xu Fachgebiet 3D-Nanostrukturierung, Institut für Physik Contact: yong.lei@tu-ilmenau.de; yang.xu@tu-ilmenau.de Office: Unterpoerlitzer

More information

KATIHAL FİZİĞİ MNT-510

KATIHAL FİZİĞİ MNT-510 KATIHAL FİZİĞİ MNT-510 YARIİLETKENLER Kaynaklar: Katıhal Fiziği, Prof. Dr. Mustafa Dikici, Seçkin Yayıncılık Katıhal Fiziği, Şakir Aydoğan, Nobel Yayıncılık, Physics for Computer Science Students: With

More information

UNIT I: Electronic Materials.

UNIT I: Electronic Materials. SIDDHARTH INSTITUTE OF ENGINEERING & TECHNOLOGY :: PUTTUR Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) Subject with Code: SEMICONDUCTOR PHYSICS (18HS0851) Course & Branch: B.Tech

More information

Contents. Preface to the first edition

Contents. Preface to the first edition Contents List of authors Preface to the first edition Introduction x xi xiii 1 The nanotechnology revolution 1 1.1 From micro- to nanoelectronics 2 1.2 From the macroscopic to the nanoscopic world 4 1.3

More information

Mesoporous titanium dioxide electrolyte bulk heterojunction

Mesoporous titanium dioxide electrolyte bulk heterojunction Mesoporous titanium dioxide electrolyte bulk heterojunction The term "bulk heterojunction" is used to describe a heterojunction composed of two different materials acting as electron- and a hole- transporters,

More information

A semiconductor is an almost insulating material, in which by contamination (doping) positive or negative charge carriers can be introduced.

A semiconductor is an almost insulating material, in which by contamination (doping) positive or negative charge carriers can be introduced. Semiconductor A semiconductor is an almost insulating material, in which by contamination (doping) positive or negative charge carriers can be introduced. Page 2 Semiconductor materials Page 3 Energy levels

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

David J. Starling Penn State Hazleton PHYS 214

David J. Starling Penn State Hazleton PHYS 214 Being virtually killed by a virtual laser in a virtual space is just as effective as the real thing, because you are as dead as you think you are. -Douglas Adams, Mostly Harmless David J. Starling Penn

More information

Review of Semiconductor Fundamentals

Review of Semiconductor Fundamentals ECE 541/ME 541 Microelectronic Fabrication Techniques Review of Semiconductor Fundamentals Zheng Yang (ERF 3017, email: yangzhen@uic.edu) Page 1 Semiconductor A semiconductor is an almost insulating material,

More information

EXTRINSIC SEMICONDUCTOR

EXTRINSIC SEMICONDUCTOR EXTRINSIC SEMICONDUCTOR EXTRINSIC SEMICONDUCTOR A semiconductor in which the impurity atoms are added by doping process is called Extrinsic semiconductor. The addition of impurities increases the carrier

More information

Fabrication Technology, Part I

Fabrication Technology, Part I EEL5225: Principles of MEMS Transducers (Fall 2004) Fabrication Technology, Part I Agenda: Microfabrication Overview Basic semiconductor devices Materials Key processes Oxidation Thin-film Deposition Reading:

More information

From Last Time Important new Quantum Mechanical Concepts. Atoms and Molecules. Today. Symmetry. Simple molecules.

From Last Time Important new Quantum Mechanical Concepts. Atoms and Molecules. Today. Symmetry. Simple molecules. Today From Last Time Important new Quantum Mechanical Concepts Indistinguishability: Symmetries of the wavefunction: Symmetric and Antisymmetric Pauli exclusion principle: only one fermion per state Spin

More information

Inorganic compounds that semiconduct tend to have an average of 4 valence electrons, and their conductivity may be increased by doping.

Inorganic compounds that semiconduct tend to have an average of 4 valence electrons, and their conductivity may be increased by doping. Chapter 12 Modern Materials 12.1 Semiconductors Inorganic compounds that semiconduct tend to have an average of 4 valence electrons, and their conductivity may be increased by doping. Doping yields different

More information

Wafer-scale fabrication of graphene

Wafer-scale fabrication of graphene Wafer-scale fabrication of graphene Sten Vollebregt, MSc Delft University of Technology, Delft Institute of Mircosystems and Nanotechnology Delft University of Technology Challenge the future Delft University

More information

Electronic Processes on Semiconductor Surfaces during Chemisorption

Electronic Processes on Semiconductor Surfaces during Chemisorption Electronic Processes on Semiconductor Surfaces during Chemisorption T. Wolkenstein Translatedfrom Russian by E. M. Yankovskii Translation edited in part by Roy Morrison CONSULTANTS BUREAU NEW YORK AND

More information

Engineering 2000 Chapter 8 Semiconductors. ENG2000: R.I. Hornsey Semi: 1

Engineering 2000 Chapter 8 Semiconductors. ENG2000: R.I. Hornsey Semi: 1 Engineering 2000 Chapter 8 Semiconductors ENG2000: R.I. Hornsey Semi: 1 Overview We need to know the electrical properties of Si To do this, we must also draw on some of the physical properties and we

More information

Stepwise Solution Important Instructions to examiners:

Stepwise Solution Important Instructions to examiners: (ISO/IEC - 700-005 Certified) WINTER 0 EXAMINATION Subject Code: 70 Model Answer (Applied Science- Physics) Page No: 0/5 No. Sub. Important Instructions to examiners: ) The answers should be examined by

More information

Multi-Layer Coating of Ultrathin Polymer Films on Nanoparticles of Alumina by a Plasma Treatment

Multi-Layer Coating of Ultrathin Polymer Films on Nanoparticles of Alumina by a Plasma Treatment Mat. Res. Soc. Symp. Vol. 635 2001 Materials Research Society Multi-Layer Coating of Ultrathin Polymer Films on Nanoparticles of Alumina by a Plasma Treatment Donglu Shi, Zhou Yu, S. X. Wang 1, Wim J.

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

EE143 Fall 2016 Microfabrication Technologies. Evolution of Devices

EE143 Fall 2016 Microfabrication Technologies. Evolution of Devices EE143 Fall 2016 Microfabrication Technologies Prof. Ming C. Wu wu@eecs.berkeley.edu 511 Sutardja Dai Hall (SDH) 1-1 Evolution of Devices Yesterday s Transistor (1947) Today s Transistor (2006) 1-2 1 Why

More information

Contents CONTENTS. Page 2 of 47

Contents CONTENTS. Page 2 of 47 J. A. Hargreaves Lockerbie Academy June 2015 Contents CONTENTS Contents... 2 CHAPTER 7 CONDUCTORS, SEMICONDUCTORS AND INSULATORS... 4 Summary of Content... 4 Summary of this chapter- notes from column

More information

So why is sodium a metal? Tungsten Half-filled 5d band & half-filled 6s band. Insulators. Interaction of metals with light?

So why is sodium a metal? Tungsten Half-filled 5d band & half-filled 6s band. Insulators. Interaction of metals with light? Bonding in Solids: Metals, Insulators, & CHEM 107 T. Hughbanks Delocalized bonding in Solids Think of a pure solid as a single, very large molecule. Use our bonding pictures to try to understand properties.

More information

Introduction to Semiconductor Physics. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India

Introduction to Semiconductor Physics. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India Introduction to Semiconductor Physics 1 Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India http://folk.uio.no/ravi/cmp2013 Review of Semiconductor Physics Semiconductor fundamentals

More information

3.23 Electrical, Optical, and Magnetic Properties of Materials

3.23 Electrical, Optical, and Magnetic Properties of Materials MIT OpenCourseWare http://ocw.mit.edu 3.23 Electrical, Optical, and Magnetic Properties of Materials Fall 2007 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms.

More information

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Professor Ali Javey. Spring 2009.

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Professor Ali Javey. Spring 2009. UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences EE143 Professor Ali Javey Spring 2009 Exam 1 Name: SID: Closed book. One sheet of notes is allowed.

More information

Chemistry Instrumental Analysis Lecture 8. Chem 4631

Chemistry Instrumental Analysis Lecture 8. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 8 UV to IR Components of Optical Basic components of spectroscopic instruments: stable source of radiant energy transparent container to hold sample device

More information

Graphene Fundamentals and Emergent Applications

Graphene Fundamentals and Emergent Applications Graphene Fundamentals and Emergent Applications Jamie H. Warner Department of Materials University of Oxford Oxford, UK Franziska Schaffel Department of Materials University of Oxford Oxford, UK Alicja

More information

CH676 Physical Chemistry: Principles and Applications. CH676 Physical Chemistry: Principles and Applications

CH676 Physical Chemistry: Principles and Applications. CH676 Physical Chemistry: Principles and Applications CH676 Physical Chemistry: Principles and Applications Crystal Structure and Chemistry Synthesis of Tetrahexahedral Platinum Nanocrystals with High-Index Facets and High Electro-Oxidation Activity Na Tian

More information

REFRACTORY METAL OXIDES: FABRICATION OF NANOSTRUCTURES, PROPERTIES AND APPLICATIONS

REFRACTORY METAL OXIDES: FABRICATION OF NANOSTRUCTURES, PROPERTIES AND APPLICATIONS REFRACTORY METAL OXIDES: FABRICATION OF NANOSTRUCTURES, PROPERTIES AND APPLICATIONS S.K. Lazarouk, D.A. Sasinovich BELARUSIAN STATE UNIVERSITY OF INFORMATICS AND RADIOELECTRONICS Outline: -- experimental

More information

Lecture 18: Semiconductors - continued (Kittel Ch. 8)

Lecture 18: Semiconductors - continued (Kittel Ch. 8) Lecture 18: Semiconductors - continued (Kittel Ch. 8) + a - Donors and acceptors J U,e e J q,e Transport of charge and energy h E J q,e J U,h Physics 460 F 2006 Lect 18 1 Outline More on concentrations

More information

The design of an integrated XPS/Raman spectroscopy instrument for co-incident analysis

The design of an integrated XPS/Raman spectroscopy instrument for co-incident analysis The design of an integrated XPS/Raman spectroscopy instrument for co-incident analysis Tim Nunney The world leader in serving science 2 XPS Surface Analysis XPS +... UV Photoelectron Spectroscopy UPS He(I)

More information

Contents. Foreword by Darrell H. Reneker

Contents. Foreword by Darrell H. Reneker Table of Foreword by Darrell H. Reneker Preface page xi xiii 1 Introduction 1 1.1 How big is a nanometer? 1 1.2 What is nanotechnology? 1 1.3 Historical development of nanotechnology 2 1.4 Classification

More information

Photocatalysis: semiconductor physics

Photocatalysis: semiconductor physics Photocatalysis: semiconductor physics Carlos J. Tavares Center of Physics, University of Minho, Portugal ctavares@fisica.uminho.pt www.fisica.uminho.pt 1 Guimarães Where do I come from? 3 Guimarães 4 Introduction>>

More information

Minimal Update of Solid State Physics

Minimal Update of Solid State Physics Minimal Update of Solid State Physics It is expected that participants are acquainted with basics of solid state physics. Therefore here we will refresh only those aspects, which are absolutely necessary

More information

Semiconductor Detectors

Semiconductor Detectors Semiconductor Detectors Summary of Last Lecture Band structure in Solids: Conduction band Conduction band thermal conductivity: E g > 5 ev Valence band Insulator Charge carrier in conductor: e - Charge

More information

EECS143 Microfabrication Technology

EECS143 Microfabrication Technology EECS143 Microfabrication Technology Professor Ali Javey Introduction to Materials Lecture 1 Evolution of Devices Yesterday s Transistor (1947) Today s Transistor (2006) Why Semiconductors? Conductors e.g

More information

Macromolecules on Nano-Outlets Responding to Electric Field and ph for Dual-Mode Drug Delivery

Macromolecules on Nano-Outlets Responding to Electric Field and ph for Dual-Mode Drug Delivery Supporting Information for: Macromolecules on Nano-Outlets Responding to Electric Field and ph for Dual-Mode Drug Delivery Fang Li, Yingchun Zhu*, Zhiyong Mao, Yunli Wang, Qichao Ruan, Jianlin Shi, Congqin

More information

EE 446/646 Photovoltaic Devices I. Y. Baghzouz

EE 446/646 Photovoltaic Devices I. Y. Baghzouz EE 446/646 Photovoltaic Devices I Y. Baghzouz What is Photovoltaics? First used in about 1890, the word has two parts: photo, derived from the Greek word for light, volt, relating to electricity pioneer

More information

Gas Sensors and Solar Water Splitting. Yang Xu

Gas Sensors and Solar Water Splitting. Yang Xu Gas Sensors and Solar Water Splitting Yang Xu 11/16/14 Seite 1 Gas Sensor 11/16/14 Seite 2 What are sensors? American National Standards Institute (ANSI) Definition: a device which provides a usable output

More information

Seminars in Nanosystems - I

Seminars in Nanosystems - I Seminars in Nanosystems - I Winter Semester 2011/2012 Dr. Emanuela Margapoti Emanuela.Margapoti@wsi.tum.de Dr. Gregor Koblmüller Gregor.Koblmueller@wsi.tum.de Seminar Room at ZNN 1 floor Topics of the

More information

FACULTY OF ENGINEERING ALEXANDRIA UNVERSITY. Solid State lab. Instructors Dr. M. Ismail El-Banna Dr. Mohamed A. El-Shimy TA Noha Hanafy

FACULTY OF ENGINEERING ALEXANDRIA UNVERSITY. Solid State lab. Instructors Dr. M. Ismail El-Banna Dr. Mohamed A. El-Shimy TA Noha Hanafy FACULTY OF ENGINEERING ALEXANDRIA UNVERSITY Solid State lab Instructors Dr. M. Ismail El-Banna Dr. Mohamed A. El-Shimy TA Noha Hanafy 2017-2018 first term A. Experiments 1- Relationship between the intensity

More information

Lecture 7: Extrinsic semiconductors - Fermi level

Lecture 7: Extrinsic semiconductors - Fermi level Lecture 7: Extrinsic semiconductors - Fermi level Contents 1 Dopant materials 1 2 E F in extrinsic semiconductors 5 3 Temperature dependence of carrier concentration 6 3.1 Low temperature regime (T < T

More information

Computational Materials Design and Discovery Energy and Electronic Applications Synthesis Structure Properties

Computational Materials Design and Discovery Energy and Electronic Applications Synthesis Structure Properties Computational Materials Design and Discovery Energy and Electronic Applications Synthesis Structure Properties Supercapacitors Rechargeable batteries Supercomputer Photocatalysts Fuel cell catalysts First

More information

Chem 481 Lecture Material 3/20/09

Chem 481 Lecture Material 3/20/09 Chem 481 Lecture Material 3/20/09 Radiation Detection and Measurement Semiconductor Detectors The electrons in a sample of silicon are each bound to specific silicon atoms (occupy the valence band). If

More information

Enhanced Photonic Properties of Thin Opaline Films as a Consequence of Embedded Nanoparticles.

Enhanced Photonic Properties of Thin Opaline Films as a Consequence of Embedded Nanoparticles. Enhanced Photonic Properties of Thin Opaline Films as a Consequence of Embedded Nanoparticles. D E Whitehead, M Bardosova and M E Pemble Tyndall National Institute, University College Cork Ireland Introduction:

More information

Plastic Electronics. Joaquim Puigdollers.

Plastic Electronics. Joaquim Puigdollers. Plastic Electronics Joaquim Puigdollers Joaquim.puigdollers@upc.edu Nobel Prize Chemistry 2000 Origins Technological Interest First products.. MONOCROMATIC PHILIPS Today Future Technological interest Low

More information

ELECTRONIC DEVICES AND CIRCUITS SUMMARY

ELECTRONIC DEVICES AND CIRCUITS SUMMARY ELECTRONIC DEVICES AND CIRCUITS SUMMARY Classification of Materials: Insulator: An insulator is a material that offers a very low level (or negligible) of conductivity when voltage is applied. Eg: Paper,

More information

ESE 372 / Spring 2013 / Lecture 5 Metal Oxide Semiconductor Field Effect Transistor

ESE 372 / Spring 2013 / Lecture 5 Metal Oxide Semiconductor Field Effect Transistor Metal Oxide Semiconductor Field Effect Transistor V G V G 1 Metal Oxide Semiconductor Field Effect Transistor We will need to understand how this current flows through Si What is electric current? 2 Back

More information

Materials and Structural Design for Advanced Energy Storage Devices

Materials and Structural Design for Advanced Energy Storage Devices Materials and Structural Design for Advanced Energy Storage Devices Imran Shakir Sustainable Energy Technologies Center (SET) King Saud University Saudi Arabia Specific Power (W/kg) Introduction and Motivation

More information

Initial Stages of Growth of Organic Semiconductors on Graphene

Initial Stages of Growth of Organic Semiconductors on Graphene Initial Stages of Growth of Organic Semiconductors on Graphene Presented by: Manisha Chhikara Supervisor: Prof. Dr. Gvido Bratina University of Nova Gorica Outline Introduction to Graphene Fabrication

More information

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

Carriers Concentration in Semiconductors - V. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India Carriers Concentration in Semiconductors - V 1 Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India http://folk.uio.no/ravi/semi2013 Motion and Recombination of Electrons and

More information

Plasma Deposition (Overview) Lecture 1

Plasma Deposition (Overview) Lecture 1 Plasma Deposition (Overview) Lecture 1 Material Processes Plasma Processing Plasma-assisted Deposition Implantation Surface Modification Development of Plasma-based processing Microelectronics needs (fabrication

More information

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626 OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Announcements HW#3 is assigned due Feb. 20 st Mid-term exam Feb 27, 2PM

More information

2D Materials for Gas Sensing

2D Materials for Gas Sensing 2D Materials for Gas Sensing S. Guo, A. Rani, and M.E. Zaghloul Department of Electrical and Computer Engineering The George Washington University, Washington DC 20052 Outline Background Structures of

More information

ECE 442. Spring, Lecture -2

ECE 442. Spring, Lecture -2 ECE 442 Power Semiconductor Devices and Integrated circuits Spring, 2006 University of Illinois at Chicago Lecture -2 Semiconductor physics band structures and charge carriers 1. What are the types of

More information

Chapter 3 Engineering Science for Microsystems Design and Fabrication

Chapter 3 Engineering Science for Microsystems Design and Fabrication Lectures on MEMS and MICROSYSTEMS DESIGN and MANUFACTURE Chapter 3 Engineering Science for Microsystems Design and Fabrication In this Chapter, we will present overviews of the principles of physical and

More information

Electro - Principles I

Electro - Principles I Electro - Principles I Page 10-1 Atomic Theory It is necessary to know what goes on at the atomic level of a semiconductor so the characteristics of the semiconductor can be understood. In many cases a

More information

Semiconductors. Semiconductors also can collect and generate photons, so they are important in optoelectronic or photonic applications.

Semiconductors. Semiconductors also can collect and generate photons, so they are important in optoelectronic or photonic applications. Semiconductors Semiconducting materials have electrical properties that fall between true conductors, (like metals) which are always highly conducting and insulators (like glass or plastic or common ceramics)

More information

Ion Implant Part 1. Saroj Kumar Patra, TFE4180 Semiconductor Manufacturing Technology. Norwegian University of Science and Technology ( NTNU )

Ion Implant Part 1. Saroj Kumar Patra, TFE4180 Semiconductor Manufacturing Technology. Norwegian University of Science and Technology ( NTNU ) 1 Ion Implant Part 1 Chapter 17: Semiconductor Manufacturing Technology by M. Quirk & J. Serda Spring Semester 2014 Saroj Kumar Patra,, Norwegian University of Science and Technology ( NTNU ) 2 Objectives

More information

Challenges in to-electric Energy Conversion: an Introduction

Challenges in to-electric Energy Conversion: an Introduction Challenges in Solar-to to-electric Energy Conversion: an Introduction Eray S. Aydil Chemical Engineering and Materials Science Department Acknowledgements: National Science Foundation Minnesota Initiative

More information

Crystalline Solids have atoms arranged in an orderly repeating pattern. Amorphous Solids lack the order found in crystalline solids

Crystalline Solids have atoms arranged in an orderly repeating pattern. Amorphous Solids lack the order found in crystalline solids Ch 12: Solids and Modern Materials Learning goals and key skills: Classify solids base on bonding/intermolecular forces and understand how difference in bonding relates to physical properties Know the

More information

Carbon Nanomaterials: Nanotubes and Nanobuds and Graphene towards new products 2030

Carbon Nanomaterials: Nanotubes and Nanobuds and Graphene towards new products 2030 Carbon Nanomaterials: Nanotubes and Nanobuds and Graphene towards new products 2030 Prof. Dr. Esko I. Kauppinen Helsinki University of Technology (TKK) Espoo, Finland Forecast Seminar February 13, 2009

More information

PV Tutorial Allen Hermann, Ph. D. Professor of Physics Emeritus, and Professor of Music Adjunct, University of Colorado, Boulder, Colorado, USA and

PV Tutorial Allen Hermann, Ph. D. Professor of Physics Emeritus, and Professor of Music Adjunct, University of Colorado, Boulder, Colorado, USA and PV Tutorial Allen Hermann, Ph. D. Professor of Physics Emeritus, and Professor of Music Adjunct, University of Colorado, Boulder, Colorado, USA and Vice-president, NanoTech Inc. Lexington, Kentucky, USA

More information

ET3034TUx Utilization of band gap energy

ET3034TUx Utilization of band gap energy ET3034TUx - 3.3.1 - Utilization of band gap energy In the last two weeks we have discussed the working principle of a solar cell and the external parameters that define the performance of a solar cell.

More information

Starting solution. Hydrolysis reaction under thermostatic conditions. Check of viscosity and deposition test SOL. Deposition by spin coating

Starting solution. Hydrolysis reaction under thermostatic conditions. Check of viscosity and deposition test SOL. Deposition by spin coating Supplementary Figures Tetramethyl orthosilicate (TMOS) Tetrahydrofuran anhydrous (THF) Trimethyl methoxy silane (TMMS) Trimethyl silil acetate (TMSA) Starting solution Hydrolysis reaction under thermostatic

More information

Nanoparticles, nanorods, nanowires

Nanoparticles, nanorods, nanowires Nanoparticles, nanorods, nanowires Nanoparticles, nanocrystals, nanospheres, quantum dots, etc. Drugs, proteins, etc. Nanorods, nanowires. Optical and electronic properties. Organization using biomolecules.

More information

3C3 Analogue Circuits

3C3 Analogue Circuits Department of Electronic & Electrical Engineering Trinity College Dublin, 2014 3C3 Analogue Circuits Prof J K Vij jvij@tcd.ie Lecture 1: Introduction/ Semiconductors & Doping 1 Course Outline (subject

More information

A Novel Electroless Method for the Deposition of Single-Crystalline Platinum Nanoparticle Films On

A Novel Electroless Method for the Deposition of Single-Crystalline Platinum Nanoparticle Films On Supplementary Information A Novel Electroless Method for the Deposition of Single-Crystalline Platinum Nanoparticle Films On an Organic Solid Matrix in the Presence of Gold Single Crystals Khaleda Banu,,,*

More information

ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems

ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Lec 6: September 18, 2017 MOS Model You are Here: Transistor Edition! Previously: simple models (0 and 1 st order) " Comfortable

More information

Organic Electronic Devices

Organic Electronic Devices Organic Electronic Devices Week 5: Organic Light-Emitting Devices and Emerging Technologies Lecture 5.5: Course Review and Summary Bryan W. Boudouris Chemical Engineering Purdue University 1 Understanding

More information

Molecules and Condensed Matter

Molecules and Condensed Matter Chapter 42 Molecules and Condensed Matter PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Goals for Chapter 42 To understand

More information

Transparent TiO 2 nanotube/nanowire arrays on TCO coated glass substrates: Synthesis and application to solar energy conversion

Transparent TiO 2 nanotube/nanowire arrays on TCO coated glass substrates: Synthesis and application to solar energy conversion Transparent TiO 2 nanotube/nanowire arrays on TCO coated glass substrates: Synthesis and application to solar energy conversion Craig A. Grimes Department of Electrical Engineering Center for Solar Nanomaterials

More information

4.2 Molecular orbitals and atomic orbitals Consider a linear chain of four identical atoms representing a hypothetical molecule.

4.2 Molecular orbitals and atomic orbitals Consider a linear chain of four identical atoms representing a hypothetical molecule. 4. Molecular orbitals and atomic orbitals Consider a linear chain of four identical atoms representing a hypothetical molecule. Suppose that each atomic wavefunction is 1s wavefunction. This system of

More information

University of Groningen. Photophysics of nanomaterials for opto-electronic applications Kahmann, Simon

University of Groningen. Photophysics of nanomaterials for opto-electronic applications Kahmann, Simon University of Groningen Photophysics of nanomaterials for opto-electronic applications Kahmann, Simon IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you wish to

More information

Lecture 2. Semiconductor Physics. Sunday 4/10/2015 Semiconductor Physics 1-1

Lecture 2. Semiconductor Physics. Sunday 4/10/2015 Semiconductor Physics 1-1 Lecture 2 Semiconductor Physics Sunday 4/10/2015 Semiconductor Physics 1-1 Outline Intrinsic bond model: electrons and holes Charge carrier generation and recombination Intrinsic semiconductor Doping:

More information

ECE 335: Electronic Engineering Lecture 2: Semiconductors

ECE 335: Electronic Engineering Lecture 2: Semiconductors Faculty of Engineering ECE 335: Electronic Engineering Lecture 2: Semiconductors Agenda Intrinsic Semiconductors Extrinsic Semiconductors N-type P-type Carrier Transport Drift Diffusion Semiconductors

More information

Imaging Carbon materials with correlative Raman-SEM microscopy. Introduction. Raman, SEM and FIB within one chamber. Diamond.

Imaging Carbon materials with correlative Raman-SEM microscopy. Introduction. Raman, SEM and FIB within one chamber. Diamond. Imaging Carbon materials with correlative Raman-SEM microscopy Application Example Carbon materials are widely used in many industries for their exceptional properties. Electric conductance, light weight,

More information

Tailored surface modification of substrates by atmospheric plasma for improved compatibility with specific adhesive Nicolas Vandencasteele

Tailored surface modification of substrates by atmospheric plasma for improved compatibility with specific adhesive Nicolas Vandencasteele 1 oating Plasma Innovation Tailored surface modification of substrates by atmospheric plasma for improved compatibility with specific adhesive Nicolas Vandencasteele 2 Plasma Applications Adhesion improvement

More information

Physical Final Exam

Physical Final Exam Physical 2 2014 Final Exam 1) When benzoic acid is added to an oil and water emulsion it will distribute itself as follows: a) dissolve only in water b) dissolve only in oil c) it will disperse in both

More information

UNIT - IV SEMICONDUCTORS AND MAGNETIC MATERIALS

UNIT - IV SEMICONDUCTORS AND MAGNETIC MATERIALS 1. What is intrinsic If a semiconductor is sufficiently pure, then it is known as intrinsic semiconductor. ex:: pure Ge, pure Si 2. Mention the expression for intrinsic carrier concentration of intrinsic

More information

Diamond. Covalent Insulators and Semiconductors. Silicon, Germanium, Gray Tin. Chem 462 September 24, 2004

Diamond. Covalent Insulators and Semiconductors. Silicon, Germanium, Gray Tin. Chem 462 September 24, 2004 Covalent Insulators and Chem 462 September 24, 2004 Diamond Pure sp 3 carbon All bonds staggered- ideal d(c-c) - 1.54 Å, like ethane Silicon, Germanium, Gray Tin Diamond structure Si and Ge: semiconductors

More information

Highly corrosion resistant organic-inorganic hybrid coatings prepared using the sol-gel process

Highly corrosion resistant organic-inorganic hybrid coatings prepared using the sol-gel process SÃO PAULO STATE UNIVERSITY- UNESP INSTITUTE OF CHEMISTRY - ARARAQUARA, BRAZIL Highly corrosion resistant organic-inorganic hybrid coatings prepared using the sol-gel process P. Hammer*, F. C. dos Santos,

More information

2011 GCEP Report. Project title: Self-sorting of Carbon Nanotubes for High Performance Large Area Transparent Electrodes for Solar Cells

2011 GCEP Report. Project title: Self-sorting of Carbon Nanotubes for High Performance Large Area Transparent Electrodes for Solar Cells 2011 GCEP Report Project title: Self-sorting of Carbon Nanotubes for High Performance Large Area Transparent Electrodes for Solar Cells Investigators Zhenan Bao, Associate Professor, Chemical Engineering

More information