SiC activities at Linköping University

Size: px
Start display at page:

Download "SiC activities at Linköping University"

Transcription

1 SiC activities at Linköping University A. Henry and E. Janzén

2 SiC : Prof. Erik Janzen growth (bulk and epi) defect and characterisation Nitride : Prof. Bo Monemar growth optical characterisation Electronic Structure : Prof. L. Johansson photoemission Spintronic : Prof. Weimin Chen Magneto-optic measurements Compound Semiconductors : Prof. Per-Olof Holtz optical characterisation

3 SiC activities Growth Bulk Sublimation High temperature CVD Epitaxy Horizontal Hot Wall CVD Vertical Hot Wall CVD Sublimation Epitaxy LPE Simulation Characterization Optical PL, PLE, Time resolved PL, FTIR, FTPL, CL Electrical Hall, IV, CV, DLTS, MCTS Magnetic resonance ODMR, EPR Structural XRD, Lang topograph Theoretical calculation S-Science : Sensor application Thin Film : TEM

4 High-Power diode SiC diodes Contacts p n Junction Termination Passivation Si IGBTs N + Substrate Active layer 2.5kV : 30 µm thick CVD n - 1.5E15 cm -3

5 Horizontal Hot-Wall CVD epilayer Quartz tube Insulation Graphite Substrate Coil Gas Inlet H 2 carrier SiH 4 + C 3 H 8 Doping (N 2, TMA ) Growth Temperature: 1600 o C in horizontal Growth Pressure: mbar O. Kordina C. Hallin : surf. prep., precursor U. Forsberg :MESFET Ö. Danielsson :Simulation

6 Simulation Ö. Danielsson Temperature Doping concentration (cm -3 ) Si-face C-face N Doping C/Si ratio Inlet C 3 H 8 flow (ml/min) Growth Rate Growth rate (µm/h) Doping concentration (cm -3 ) mbar 13 l/min Position along gas flow direction (mm) Inlet C 3 H 8 flow (ml/min) Si-face C-face Inlet SiH 4 flow (ml/min)

7 Degradation : Drift of the forward current 200 Virgin device Intermediate Stressed Creation and expansion of stacking faults Cathodoluminescence CL X-ray Topography 150 Ja[A/cm2] ,5 3 3,5 4 4,5 Va[V] P. Bergman

8 P. Bergman Lang topo [1,-1,] PL at 77K Cathodoluminescence CL X-ray Topography 6 x 4 5 Low Temperature PL Normal Spectra New Defect Emission PL Intensity Photon Wavelength (nm)

9 Today (2 inch diam) Thickness typically µm (80 µm) Unif = σ/mean < 8% Background doping level n-type (nitrogen) 1-2E14 N-doping 1E15 5E18 Unif < 20% Al-doping 5E15 1E19 Unif <20% Typical lifetime (35 um, 2E15) > 250 µs Future work related to SiC-CVD - Degradation : reduction of critical defects - Lifetime limiting defects - growth on non-standard surface - δ-doped layers - Regrowth - Other dopant : P, As, B, V

10 High Temperature CVD Bulk Seeded Sublimation Growth O. Kordina A. Ellison Insulation 1 Seed Crystal RF Coil RF Coil Source T process: C Seed Heater Crucible Quartz tube Graphite Foam HTCVD advantages: high vacuum high purity of the sources gases continuous supply of the source material possibility to adjust C/Si Gas Inlet Helium carrier SiH + C H 4 2 4

11 Id (ma) High Frequency Device SiC MESFET with Commercial S.I. substrate Degradation of I-V static characteristics Vgs=0V, -2V/step I DS (ma) V GS = 0 V SiC MESFET with PURER SUBSTRATE (HTCVD) (80 V STRESS) I DS (V DS ) Light ON Light OFF MESFET 1 0 µm V GS = -2 V/step Vds (V) V DS (V) C. Brilinski ECSCRM JESICA PROJECT

12 2-inch diameter 4H-SiC substrates pilot products SI on- and off-axis P+ N+ off-axis off-axis

13 Future work related to HTCVD Characterization : - identification of defects in SI SiC and understand their properties - Support to Okmetic (SI, N and P substrates)

14 Characterization Most studied defects in SiC after irradiation / implantation and annealing (2 MeV T>1200 C) Optical Electrical D 1 : Speudo-donor Z 1,2 PL intensity (arb.units) PL L 1 1S (T. Egilsson) PLE M 1 1 E C L 1 62 mev Photon Energy (mev) 2S 3S4S S-like P-like 0 P -like +/ - series limit 4H-SiC C/C (arb. units) HS1 E V ev MCTS (hole trap) DLTS (e lectron trap ) Z ½ E C ev 4H -SiC Temperatu re (K) (L. Storasta)

15 - Association D1 HS1-3 Z 1/2 (cm ) -3 HS1 (cm ) PL L /Q Annealing temperature ( C) (L. Storasta) - 3 DLTS & MCTS concentrat ion (cm ) 4H Si C PL L /Q s, 2p 1s L ev CB 2.9 ev VB 62 mev HS1

16 Characterization Defect study : Atom displacement C : 90 kev Si: 220 kev Face dependent? N-type 2.5E15 cm -3 epi Low energy electron irradiation kev L. Storatas DLTS/MCTS signal (arb.units) Electron traps Hole traps HS2 EH1 Z 1/2 EH3 DLTS MCTS EH Temperature (K)

17 Si-face 4H epilayer Introduction rate (arb.units) HS2 EH1 EH6 EH3 Z 1/2 C/Si face concentration ratio 1 EH1, EH3, Z 1/2 HS Irradiation energy (kev) Irradiation energy (kev) L. Storatas C related centers

18 Photoluminescence F. Carlsson PL Intensity (a.u.) log(plintensity) (a.u.) 5 4 L 1 L 1 g 2 g 2 g 1 g 1 f1 e1 e kev 160 kev TEM electrons 120keV c 2 d 1 c 1 d 1 c 2 c 1 b1 b 1 Si-Side Si-side a 1 C-Side C-side Wavelength ( Å) Wavelength (Å) a 1 PL Intensity (a.u.) PL Intensity (a.u.) L 1 L 1 g 2 g 1 g 2 g 1 e2 e 1 e 1 c 2 d 1 c 1 c 1 d1 c 2 PCB990 min TEM irradiation 160keV b 1 b 1 a 1 a 1 d 1 phonon band c 1 phonon band Si-Side b 1 phonon band b 1 (78meV) b 1 phonon band b 1 (78meV) Wavelength (Å) Wavelength (Å) 4H-SiC T=2K Si-side C-side C-Side

Optical Hyperdoping: Transforming Semiconductor Band Structure for Solar Energy Harvesting

Optical Hyperdoping: Transforming Semiconductor Band Structure for Solar Energy Harvesting Optical Hyperdoping: Transforming Semiconductor Band Structure for Solar Energy Harvesting 3G Solar Technologies Multidisciplinary Workshop MRS Spring Meeting San Francisco, CA, 5 April 2010 Michael P.

More information

Conductivity of silicon can be changed several orders of magnitude by introducing impurity atoms in silicon crystal lattice.

Conductivity of silicon can be changed several orders of magnitude by introducing impurity atoms in silicon crystal lattice. CMOS Processing Technology Silicon: a semiconductor with resistance between that of conductor and an insulator. Conductivity of silicon can be changed several orders of magnitude by introducing impurity

More information

High. Thickness. epitaxial Silicon. Carbide Detectors. INFN - Gruppo V 2009

High. Thickness. epitaxial Silicon. Carbide Detectors. INFN - Gruppo V 2009 INFN - Gruppo V Proposta di nuovo esperimento per il triennio 2007-2009 2009 High Thickness epitaxial Silicon Carbide Detectors Sezioni INFN di Milano - Bologna - Catania Outline A general introduction

More information

Introduction to VLSI Fabrication Technologies. Emanuele Baravelli

Introduction to VLSI Fabrication Technologies. Emanuele Baravelli Introduction to VLSI Fabrication Technologies Emanuele Baravelli 27/09/2005 Organization Materials Used in VLSI Fabrication VLSI Fabrication Technologies Overview of Fabrication Methods Device simulation

More information

Types of Epitaxy. Homoepitaxy. Heteroepitaxy

Types of Epitaxy. Homoepitaxy. Heteroepitaxy Epitaxy Epitaxial Growth Epitaxy means the growth of a single crystal film on top of a crystalline substrate. For most thin film applications (hard and soft coatings, optical coatings, protective coatings)

More information

Semiconductor doping. Si solar Cell

Semiconductor doping. Si solar Cell Semiconductor doping Si solar Cell Two Levels of Masks - photoresist, alignment Etch and oxidation to isolate thermal oxide, deposited oxide, wet etching, dry etching, isolation schemes Doping - diffusion/ion

More information

h e l p s y o u C O N T R O L

h e l p s y o u C O N T R O L contamination analysis for compound semiconductors ANALYTICAL SERVICES B u r i e d d e f e c t s, E v a n s A n a l y t i c a l g r o u p h e l p s y o u C O N T R O L C O N T A M I N A T I O N Contamination

More information

Solid State Detectors = Semi-Conductor based Detectors

Solid State Detectors = Semi-Conductor based Detectors Solid State Detectors = Semi-Conductor based Detectors Materials and their properties Energy bands and electronic structure Charge transport and conductivity Boundaries: the p-n junction Charge collection

More information

A Remote Plasma Sputter Process for High Rate Web Coating of Low Temperature Plastic Film with High Quality Thin Film Metals and Insulators

A Remote Plasma Sputter Process for High Rate Web Coating of Low Temperature Plastic Film with High Quality Thin Film Metals and Insulators A Remote Plasma Sputter Process for High Rate Web Coating of Low Temperature Plastic Film with High Quality Thin Film Metals and Insulators Dr Peter Hockley and Professor Mike Thwaites, Plasma Quest Limited

More information

Graphene a material for the future

Graphene a material for the future Graphene a material for the future by Olav Thorsen What is graphene? What is graphene? Simply put, it is a thin layer of pure carbon What is graphene? Simply put, it is a thin layer of pure carbon It has

More information

Lezioni di Tecnologie e Materiali per l Elettronica

Lezioni di Tecnologie e Materiali per l Elettronica Lezioni di Tecnologie e Materiali per l Elettronica Danilo Manstretta [email protected] microlab.unipv.it Outline Passive components Resistors Capacitors Inductors Printed circuits technologies

More information

Silicon Sensors for CMS Tracker at High-Luminosity Environment - Challenges in particle detection -

Silicon Sensors for CMS Tracker at High-Luminosity Environment - Challenges in particle detection - [email protected] Finnish Society for Natural Philosophy, Helsinki, 17 February 2015 Silicon Sensors for CMS Tracker at High-Luminosity Environment - Challenges in particle detection - Timo Peltola

More information

Broadband THz Generation from Photoconductive Antenna

Broadband THz Generation from Photoconductive Antenna Progress In Electromagnetics Research Symposium 2005, Hangzhou, China, August 22-26 331 Broadband THz Generation from Photoconductive Antenna Qing Chang 1, Dongxiao Yang 1,2, and Liang Wang 1 1 Zhejiang

More information

NANO SILICON DOTS EMBEDDED SIO 2 /SIO 2 MULTILAYERS FOR PV HIGH EFFICIENCY APPLICATION

NANO SILICON DOTS EMBEDDED SIO 2 /SIO 2 MULTILAYERS FOR PV HIGH EFFICIENCY APPLICATION NANO SILICON DOTS EMBEDDED SIO 2 /SIO 2 MULTILAYERS FOR PV HIGH EFFICIENCY APPLICATION Olivier Palais, Damien Barakel, David Maestre, Fabrice Gourbilleau and Marcel Pasquinelli 1 Outline Photovoltaic today

More information

Applied Physics of solar energy conversion

Applied Physics of solar energy conversion Applied Physics of solar energy conversion Conventional solar cells, and how lazy thinking can slow you down Some new ideas *************************************************************** Our work on semiconductor

More information

Hard Condensed Matter WZI

Hard Condensed Matter WZI Hard Condensed Matter WZI Tom Gregorkiewicz University of Amsterdam VU-LaserLab Dec 10, 2015 Hard Condensed Matter Cluster Quantum Matter Optoelectronic Materials Quantum Matter Amsterdam Mark Golden Anne

More information

FUNDAMENTAL PROPERTIES OF SOLAR CELLS

FUNDAMENTAL PROPERTIES OF SOLAR CELLS FUNDAMENTAL PROPERTIES OF SOLAR CELLS January 31, 2012 The University of Toledo, Department of Physics and Astronomy SSARE, PVIC Principles and Varieties of Solar Energy (PHYS 4400) and Fundamentals of

More information

WŝŽŶĞĞƌŝŶŐ > ĞdžƉĞƌŝĞŶĐĞ ƐŝŶĐĞ ϭϵϳϰ WŝĐŽƐƵŶ ^he > Ρ ZͲƐĞƌŝĞƐ > ƐLJƐƚĞŵƐ ƌŝěőŝŷő ƚśğ ŐĂƉ ďğƚǁğğŷ ƌğɛğăƌđś ĂŶĚ ƉƌŽĚƵĐƟŽŶ d, &hdhz K& d,/e &/>D /^, Z

WŝŽŶĞĞƌŝŶŐ > ĞdžƉĞƌŝĞŶĐĞ ƐŝŶĐĞ ϭϵϳϰ WŝĐŽƐƵŶ ^he > Ρ ZͲƐĞƌŝĞƐ > ƐLJƐƚĞŵƐ ƌŝěőŝŷő ƚśğ ŐĂƉ ďğƚǁğğŷ ƌğɛğăƌđś ĂŶĚ ƉƌŽĚƵĐƟŽŶ d, &hdhz K& d,/e &/>D /^, Z The ALD Powerhouse Picosun Defining the future of ALD Picosun s history and background date back to the very beginning of the field of atomic layer deposition. ALD was invented in Finland in 1974 by Dr.

More information

MOS (metal-oxidesemiconductor) 李 2003/12/19

MOS (metal-oxidesemiconductor) 李 2003/12/19 MOS (metal-oxidesemiconductor) 李 2003/12/19 Outline Structure Ideal MOS The surface depletion region Ideal MOS curves The SiO 2 -Si MOS diode (real case) Structure A basic MOS consisting of three layers.

More information

Chapter 5. Second Edition ( 2001 McGraw-Hill) 5.6 Doped GaAs. Solution

Chapter 5. Second Edition ( 2001 McGraw-Hill) 5.6 Doped GaAs. Solution Chapter 5 5.6 Doped GaAs Consider the GaAs crystal at 300 K. a. Calculate the intrinsic conductivity and resistivity. Second Edition ( 2001 McGraw-Hill) b. In a sample containing only 10 15 cm -3 ionized

More information

The Physics of Energy sources Renewable sources of energy. Solar Energy

The Physics of Energy sources Renewable sources of energy. Solar Energy The Physics of Energy sources Renewable sources of energy Solar Energy B. Maffei [email protected] Renewable sources 1 Solar power! There are basically two ways of using directly the radiative

More information

Dose enhancement near metal electrodes in diamond X- ray detectors. A. Lohstroh*, and D. Alamoudi

Dose enhancement near metal electrodes in diamond X- ray detectors. A. Lohstroh*, and D. Alamoudi Dose enhancement near metal electrodes in diamond X- ray detectors Acknowledgements Surrey University: P.J. Sellin M. Abd-El Rahman P. Veeramani H. Al-Barakaty F. Schirru Mechanical Workshop A. Lohstroh*,

More information

NANOSTRUCTURED ZnO AND ZAO TRANSPARENT THIN FILMS BY SPUTTERING SURFACE CHARACTERIZATION

NANOSTRUCTURED ZnO AND ZAO TRANSPARENT THIN FILMS BY SPUTTERING SURFACE CHARACTERIZATION Rev.Adv.Mater.Sci. Nanostructured ZnO 10 and (2005) ZAO 335-340 transparent thin films by sputtering surface characterization 335 NANOSTRUCTURED ZnO AND ZAO TRANSPARENT THIN FILMS BY SPUTTERING SURFACE

More information

Advanced VLSI Design CMOS Processing Technology

Advanced VLSI Design CMOS Processing Technology Isolation of transistors, i.e., their source and drains, from other transistors is needed to reduce electrical interactions between them. For technologies

More information

Solar Photovoltaic (PV) Cells

Solar Photovoltaic (PV) Cells Solar Photovoltaic (PV) Cells A supplement topic to: Mi ti l S Micro-optical Sensors - A MEMS for electric power generation Science of Silicon PV Cells Scientific base for solar PV electric power generation

More information

Luminescence study of structural changes induced by laser cutting in diamond films

Luminescence study of structural changes induced by laser cutting in diamond films Luminescence study of structural changes induced by laser cutting in diamond films A. Cremades and J. Piqueras Departamento de Fisica de Materiales, Facultad de Fisicas, Universidad Complutense, 28040

More information

Figure 10.1. Process flow from starting material to polished wafer.

Figure 10.1. Process flow from starting material to polished wafer. Figure 10.1. Process flow from starting material to polished wafer. 1/11/003 Ettore Vittone- Fisica dei Semiconduttori - Lectio XI 1 Starting material: silicon dioxide (SiO ): pure form of sand (quartzite)

More information

Gamma and X-Ray Detection

Gamma and X-Ray Detection Gamma and X-Ray Detection DETECTOR OVERVIEW The kinds of detectors commonly used can be categorized as: a. Gas-filled Detectors b. Scintillation Detectors c. Semiconductor Detectors The choice of a particular

More information

DOE Solar Energy Technologies Program Peer Review. Denver, Colorado April 17-19, 2007

DOE Solar Energy Technologies Program Peer Review. Denver, Colorado April 17-19, 2007 DOE Solar Energy Technologies Program Peer Review Evaluation of Nanocrystalline Silicon Thin Film by Near-Field Scanning Optical Microscopy AAT-2-31605-05 Magnus Wagener and George Rozgonyi North Carolina

More information

CVD SILICON CARBIDE. CVD SILICON CARBIDE s attributes include:

CVD SILICON CARBIDE. CVD SILICON CARBIDE s attributes include: CVD SILICON CARBIDE CVD SILICON CARBIDE is the ideal performance material for design engineers. It outperforms conventional forms of silicon carbide, as well as other ceramics, quartz, and metals in chemical

More information

organismos internacionales

organismos internacionales Semiconductores de potencia de gap ancho en organismos internacionales Philippe Godignon & Power devices and Systems Group Systems Integration Department Centro Nacional de Microelectrónica, CNM CNM-CSIC,

More information

Graduate Student Presentations

Graduate Student Presentations Graduate Student Presentations Dang, Huong Chip packaging March 27 Call, Nathan Thin film transistors/ liquid crystal displays April 4 Feldman, Ari Optical computing April 11 Guerassio, Ian Self-assembly

More information

Lecture 12. Physical Vapor Deposition: Evaporation and Sputtering Reading: Chapter 12. ECE 6450 - Dr. Alan Doolittle

Lecture 12. Physical Vapor Deposition: Evaporation and Sputtering Reading: Chapter 12. ECE 6450 - Dr. Alan Doolittle Lecture 12 Physical Vapor Deposition: Evaporation and Sputtering Reading: Chapter 12 Evaporation and Sputtering (Metalization) Evaporation For all devices, there is a need to go from semiconductor to metal.

More information

Quantitative Photoluminescence. Studies in. a-si:h/c-si Solar Cells

Quantitative Photoluminescence. Studies in. a-si:h/c-si Solar Cells Quantitative Photoluminescence Studies in a-si:h/c-si Solar Cells Von der Fakultät für Mathematik und Naturwissenschaften der Carl von Ossietzky Universität Oldenburg zur Erlangung des Grades und Titels

More information

High power picosecond lasers enable higher efficiency solar cells.

High power picosecond lasers enable higher efficiency solar cells. White Paper High power picosecond lasers enable higher efficiency solar cells. The combination of high peak power and short wavelength of the latest industrial grade Talisker laser enables higher efficiency

More information

How MOCVD. Works Deposition Technology for Beginners

How MOCVD. Works Deposition Technology for Beginners How MOCVD Works Deposition Technology for Beginners Contents MOCVD for Beginners...3 MOCVD A Definition...4 Planetary Reactor Technology...5 Close Coupled Showerhead Technology...6 AIXTRON MOCVD Production

More information

The study of deep-level emission center in ZnO films grown on c-al 2 O 3 substrates

The study of deep-level emission center in ZnO films grown on c-al 2 O 3 substrates The study of deep-level emission center in ZnO films grown on c-al 2 O 3 substrates Guotong Du Yuantao Zhang, Jinzhong Wang, Yongguo Cui (College of Electronic Science and Engineering, State Key Laboratory

More information

The Application of Density Functional Theory in Materials Science

The Application of Density Functional Theory in Materials Science The Application of Density Functional Theory in Materials Science Slide 1 Outline Atomistic Modelling Group at MUL Density Functional Theory Numerical Details HPC Cluster at the MU Leoben Applications

More information

Arizona Institute for Renewable Energy & the Solar Power Laboratories

Arizona Institute for Renewable Energy & the Solar Power Laboratories Arizona Institute for Renewable Energy & the Solar Power Laboratories International Photovoltaic Reliability Workshop July 29-31, Tempe AZ Christiana Honsberg, Stephen Goodnick, Stuart Bowden Arizona State

More information

Radiation Enhanced Diffusion of Nickel in Silicon Diodes

Radiation Enhanced Diffusion of Nickel in Silicon Diodes Radiation Enhanced Diffusion of Nickel in Silicon Diodes J. Vobecký, P. Hazdra, V. Záhlava, ISPS, August 2012, Prague, Czech Republic Copyright [2012] IEEE. Reprinted from the Internacional Seminar on

More information

Lecture 3: Optical Properties of Bulk and Nano. 5 nm

Lecture 3: Optical Properties of Bulk and Nano. 5 nm Lecture 3: Optical Properties of Bulk and Nano 5 nm The Previous Lecture Origin frequency dependence of χ in real materials Lorentz model (harmonic oscillator model) 0 e - n( ) n' n '' n ' = 1 + Nucleus

More information

Physical Properties and Functionalization of Low-Dimensional Materials

Physical Properties and Functionalization of Low-Dimensional Materials Physical Properties and Functionalization of Low-Dimensional Materials Physics Department, University of Trieste Graduate School of Physics, XXVI cycle Supervisor: Co-supervisor: Prof. Alessandro BARALDI

More information

OLED display. Ying Cao

OLED display. Ying Cao OLED display Ying Cao Outline OLED basics OLED display A novel method of fabrication of flexible OLED display Potentials of OLED Suitable for thin, lightweight, printable displays Broad color range Good

More information

Semiconductors, diodes, transistors

Semiconductors, diodes, transistors Semiconductors, diodes, transistors (Horst Wahl, QuarkNet presentation, June 2001) Electrical conductivity! Energy bands in solids! Band structure and conductivity Semiconductors! Intrinsic semiconductors!

More information

USING OPTICAL EMISSION SPECTROSCOPY TO IMPROVE EQUIPMENT UPTIME FOR AN AL2O3 ALD PROCESS *

USING OPTICAL EMISSION SPECTROSCOPY TO IMPROVE EQUIPMENT UPTIME FOR AN AL2O3 ALD PROCESS * USING OPTICAL EMISSION SPECTROSCOPY TO IMPROVE EQUIPMENT UPTIME FOR AN AL2O3 ALD PROCESS * JOHN LOO Samsung Austin Semiconductor 12100 Samsung Blvd. Austin, Texas 78754 * Presented at the AVS 5 th International

More information

CONTENTS. Preface. 1.1.2. Energy bands of a crystal (intuitive approach)

CONTENTS. Preface. 1.1.2. Energy bands of a crystal (intuitive approach) CONTENTS Preface. Energy Band Theory.. Electron in a crystal... Two examples of electron behavior... Free electron...2. The particle-in-a-box approach..2. Energy bands of a crystal (intuitive approach)..3.

More information

Neuere Entwicklungen zur Herstellung optischer Schichten durch reaktive. Wolfgang Hentsch, Dr. Reinhard Fendler. FHR Anlagenbau GmbH

Neuere Entwicklungen zur Herstellung optischer Schichten durch reaktive. Wolfgang Hentsch, Dr. Reinhard Fendler. FHR Anlagenbau GmbH Neuere Entwicklungen zur Herstellung optischer Schichten durch reaktive Sputtertechnologien Wolfgang Hentsch, Dr. Reinhard Fendler FHR Anlagenbau GmbH Germany Contents: 1. FHR Anlagenbau GmbH in Brief

More information

Coating Thickness and Composition Analysis by Micro-EDXRF

Coating Thickness and Composition Analysis by Micro-EDXRF Application Note: XRF Coating Thickness and Composition Analysis by Micro-EDXRF www.edax.com Coating Thickness and Composition Analysis by Micro-EDXRF Introduction: The use of coatings in the modern manufacturing

More information

Vacuum Evaporation Recap

Vacuum Evaporation Recap Sputtering Vacuum Evaporation Recap Use high temperatures at high vacuum to evaporate (eject) atoms or molecules off a material surface. Use ballistic flow to transport them to a substrate and deposit.

More information

CSCI 4974 / 6974 Hardware Reverse Engineering. Lecture 8: Microscopy and Imaging

CSCI 4974 / 6974 Hardware Reverse Engineering. Lecture 8: Microscopy and Imaging CSCI 4974 / 6974 Hardware Reverse Engineering Lecture 8: Microscopy and Imaging Data Acquisition for RE Microscopy Imaging Registration and stitching Microscopy Optical Electron Scanning Transmission Scanning

More information

Reliability investigations Lifetime measurements and degradation mechanisms

Reliability investigations Lifetime measurements and degradation mechanisms Reliability investigations Lifetime measurements and degradation mechanisms Bernd Sumpf, Ute Zeimer, Karl Häusler, Andreas Klehr Ferdinand-Braun-Institut für Höchstfrequenztechnik Gustav-Kirchhoff-Straße

More information

Silicon, the test mass substrate of tomorrow? Jerome Degallaix The Next Detectors for Gravitational Wave Astronomy Beijing - 2015

Silicon, the test mass substrate of tomorrow? Jerome Degallaix The Next Detectors for Gravitational Wave Astronomy Beijing - 2015 Silicon, the test mass substrate of tomorrow? Jerome Degallaix The Next Detectors for Gravitational Wave Astronomy Beijing - 2015 Program of the talk... What we have now What we know about silicon What

More information

Novel inkjettable copper ink utilizing processing temperatures under 100 degrees C without the need of inert atmosphere

Novel inkjettable copper ink utilizing processing temperatures under 100 degrees C without the need of inert atmosphere Novel inkjettable copper ink utilizing processing temperatures under 100 degrees C without the need of inert atmosphere Printed Electronics Europe April 7-8, 2009 Dresden, Germany Dr. Zvi Yaniv Applied

More information

High Open Circuit Voltage of MQW Amorphous Silicon Photovoltaic Structures

High Open Circuit Voltage of MQW Amorphous Silicon Photovoltaic Structures High Open Circuit Voltage of MQW Amorphous Silicon Photovoltaic Structures ARGYRIOS C. VARONIDES Physics and EE Department University of Scranton 800 Linden Street, Scranton PA, 18510 United States Abstract:

More information

CRYSTAL DEFECTS: Point defects

CRYSTAL DEFECTS: Point defects CRYSTAL DEFECTS: Point defects Figure 10.15. Point defects. (a) Substitutional impurity. (b) Interstitial impurity. (c) Lattice vacancy. (d) Frenkeltype defect. 9 10/11/004 Ettore Vittone- Fisica dei Semiconduttori

More information

Exciton dissociation in solar cells:

Exciton dissociation in solar cells: Exciton dissociation in solar cells: Xiaoyang Zhu Department of Chemistry University of Minnesota, Minneapolis t (fs) 3h! E, k h! Pc Bi e - 1 Acknowledgement Organic semiconductors: Mutthias Muntwiler,

More information

Al 2 O 3, Its Different Molecular Structures, Atomic Layer Deposition, and Dielectrics

Al 2 O 3, Its Different Molecular Structures, Atomic Layer Deposition, and Dielectrics Al 2 O 3, Its Different Molecular Structures, Atomic Layer Deposition, and Dielectrics Mark Imus Douglas Sisk, Ph.D., Mentor Marian High School RET Program University of Notre Dame Project Proposal Tunneling

More information

Chemical Synthesis. Overview. Chemical Synthesis of Nanocrystals. Self-Assembly of Nanocrystals. Example: Cu 146 Se 73 (PPh 3 ) 30

Chemical Synthesis. Overview. Chemical Synthesis of Nanocrystals. Self-Assembly of Nanocrystals. Example: Cu 146 Se 73 (PPh 3 ) 30 Chemical Synthesis Spontaneous organization of molecules into stable, structurally well-defined aggregates at the nanometer length scale. Overview The 1-100 nm nanoscale length is in between traditional

More information

CryoEDM A Cryogenic Neutron-EDM Experiment. Collaboration: Sussex University, RAL, ILL, Kure University, Oxford University Hans Kraus

CryoEDM A Cryogenic Neutron-EDM Experiment. Collaboration: Sussex University, RAL, ILL, Kure University, Oxford University Hans Kraus CryoEDM A Cryogenic Neutron-EDM Experiment Collaboration: Sussex University, RAL, ILL, Kure University, Oxford University Hans Kraus nedm Overview Theoretical Background The Method of Ramsey Resonance

More information

III. Wet and Dry Etching

III. Wet and Dry Etching III. Wet and Dry Etching Method Environment and Equipment Advantage Disadvantage Directionality Wet Chemical Solutions Atmosphere, Bath 1) Low cost, easy to implement 2) High etching rate 3) Good selectivity

More information

For Touch Panel and LCD Sputtering/PECVD/ Wet Processing

For Touch Panel and LCD Sputtering/PECVD/ Wet Processing production Systems For Touch Panel and LCD Sputtering/PECVD/ Wet Processing Pilot and Production Systems Process Solutions with over 20 Years of Know-how Process Technology at a Glance for Touch Panel,

More information

Preparation of ZnS and SnS Nanopowders by Modified SILAR Technique

Preparation of ZnS and SnS Nanopowders by Modified SILAR Technique Journal of Physical Sciences, Vol. 13, 009, 9-34 ISSN: 097-8791 : www.vidyasagar.ac.in/journal Preparation of ZnS and SnS Nanopowders by Modified SILAR Technique Department of Physics The University of

More information

Coating Technology: Evaporation Vs Sputtering

Coating Technology: Evaporation Vs Sputtering Satisloh Italy S.r.l. Coating Technology: Evaporation Vs Sputtering Gianni Monaco, PhD R&D project manager, Satisloh Italy 04.04.2016 V1 The aim of this document is to provide basic technical information

More information

Nanometer-scale imaging and metrology, nano-fabrication with the Orion Helium Ion Microscope

Nanometer-scale imaging and metrology, nano-fabrication with the Orion Helium Ion Microscope [email protected] Nanometer-scale imaging and metrology, nano-fabrication with the Orion Helium Ion Microscope Bin Ming, András E. Vladár and Michael T. Postek National Institute of Standards and Technology

More information

Electron Beam and Sputter Deposition Choosing Process Parameters

Electron Beam and Sputter Deposition Choosing Process Parameters Electron Beam and Sputter Deposition Choosing Process Parameters General Introduction The choice of process parameters for any process is determined not only by the physics and/or chemistry of the process,

More information

How To Implant Anneal Ion Beam

How To Implant Anneal Ion Beam ROCHESTER INSTITUTE OF TECHNOLOGY MICROELECTRONIC ENGINEERING MEMS Ion Implant Dr. Lynn Fuller webpage: http://people.rit.edu/lffeee Electrical and Microelectronic Engineering Rochester Institute of Technology

More information

1. Photon Beam Damage and Charging at Solid Surfaces John H. Thomas III

1. Photon Beam Damage and Charging at Solid Surfaces John H. Thomas III 1. Photon Beam Damage and Charging at Solid Surfaces John H. Thomas III 1. Introduction............................. 2. Electrostatic Charging of Samples in Photoemission Experiments............................

More information

Avalanche Photodiodes: A User's Guide

Avalanche Photodiodes: A User's Guide !"#$%& Abstract Avalanche Photodiodes: A User's Guide Avalanche photodiode detectors have and will continue to be used in many diverse applications such as laser range finders and photon correlation studies.

More information

How To Understand Light And Color

How To Understand Light And Color PRACTICE EXAM IV P202 SPRING 2004 1. In two separate double slit experiments, an interference pattern is observed on a screen. In the first experiment, violet light (λ = 754 nm) is used and a second-order

More information

Silicon Wafer Solar Cells

Silicon Wafer Solar Cells Silicon Wafer Solar Cells Armin Aberle Solar Energy Research Institute of Singapore (SERIS) National University of Singapore (NUS) April 2009 1 1. PV Some background Photovoltaics (PV): Direct conversion

More information

Short overview of TEUFEL-project

Short overview of TEUFEL-project Short overview of TEUFEL-project ELAN-meeting may 2004 Frascati (I) Contents Overview of TEUFEL project at Twente Photo cathode research Recent experience Outlook Overview FEL Drive laser Photo cathode

More information

Electronic transport properties of nano-scale Si films: an ab initio study

Electronic transport properties of nano-scale Si films: an ab initio study Electronic transport properties of nano-scale Si films: an ab initio study Jesse Maassen, Youqi Ke, Ferdows Zahid and Hong Guo Department of Physics, McGill University, Montreal, Canada Motivation (of

More information

Physics 441/2: Transmission Electron Microscope

Physics 441/2: Transmission Electron Microscope Physics 441/2: Transmission Electron Microscope Introduction In this experiment we will explore the use of transmission electron microscopy (TEM) to take us into the world of ultrasmall structures. This

More information

Tecnologie convenzionali nell approccio top-down; I: metodi e problematiche per la deposizione di film sottili

Tecnologie convenzionali nell approccio top-down; I: metodi e problematiche per la deposizione di film sottili LS Scienza dei Materiali - a.a. 2005/06 Fisica delle Nanotecnologie part 8 Version 4, Dec 2005 Francesco Fuso, tel 0502214305, 0502214293 - [email protected] http://www.df.unipi.it/~fuso/dida Tecnologie

More information

Photochromism of vacancy-related centres in diamond

Photochromism of vacancy-related centres in diamond J. Phys.: Condens. Matter 12 (2000) 189 199. Printed in the UK PII: S0953-8984(00)06853-3 Photochromism of vacancy-related centres in diamond K Iakoubovskii, G J Adriaenssens and M Nesladek Laboratorium

More information

INFRARED MONITORING OF 110 GHz GYROTRON WINDOWS AT DIII D

INFRARED MONITORING OF 110 GHz GYROTRON WINDOWS AT DIII D GA A23981 INFRARED MONITORING OF 110 GHz GYROTRON WINDOWS AT DIII D by Y. GORELOV, J. LOHR, R.W. CALLIS, and D. PONCE MAY 2002 DISCLAIMER This report was prepared as an account of work sponsored by an

More information

The CVD diamond booklet

The CVD diamond booklet available at: www.diamond-materials.com/download Content 1. General properties of diamond... 2 2. Optical Properties... 4 Optical transparency...4 Absorption coefficient at 10.6 µm...5 Refractive index:

More information

Solar Cell Parameters and Equivalent Circuit

Solar Cell Parameters and Equivalent Circuit 9 Solar Cell Parameters and Equivalent Circuit 9.1 External solar cell parameters The main parameters that are used to characterise the performance of solar cells are the peak power P max, the short-circuit

More information

Lecture 3: Optical Properties of Bulk and Nano. 5 nm

Lecture 3: Optical Properties of Bulk and Nano. 5 nm Lecture 3: Optical Properties of Bulk and Nano 5 nm First H/W#1 is due Sept. 10 Course Info The Previous Lecture Origin frequency dependence of χ in real materials Lorentz model (harmonic oscillator model)

More information

Surface characterization of oxygen deficient SrTiO 3

Surface characterization of oxygen deficient SrTiO 3 U. Scotti di Uccio Surface characterization of oxygen deficient SrTiO 3 films and single crystals Coherentia-CNR-INFM Napoli, Italy Prof. R. Vaglio R. Di Capua, G. De Luca, M. Radovic, N. Lampis, P. Perna,

More information

THIN FILM MATERIALS TECHNOLOGY

THIN FILM MATERIALS TECHNOLOGY THIN FILM MATERIALS TECHNOLOGY Sputtering of Compound Materials by Kiyotaka Wasa Yokohama City University Yokohama, Japan Makoto Kitabatake Matsushita Electric Industrial Co., Ltd. Kyoto, Japan Hideaki

More information

Solid-State Physics: The Theory of Semiconductors (Ch. 10.6-10.8) SteveSekula, 30 March 2010 (created 29 March 2010)

Solid-State Physics: The Theory of Semiconductors (Ch. 10.6-10.8) SteveSekula, 30 March 2010 (created 29 March 2010) Modern Physics (PHY 3305) Lecture Notes Modern Physics (PHY 3305) Lecture Notes Solid-State Physics: The Theory of Semiconductors (Ch. 10.6-10.8) SteveSekula, 30 March 2010 (created 29 March 2010) Review

More information

Chapter 1 Introduction to The Semiconductor Industry 2005 VLSI TECH. 1

Chapter 1 Introduction to The Semiconductor Industry 2005 VLSI TECH. 1 Chapter 1 Introduction to The Semiconductor Industry 1 The Semiconductor Industry INFRASTRUCTURE Industry Standards (SIA, SEMI, NIST, etc.) Production Tools Utilities Materials & Chemicals Metrology Tools

More information

ELEC 3908, Physical Electronics, Lecture 15. BJT Structure and Fabrication

ELEC 3908, Physical Electronics, Lecture 15. BJT Structure and Fabrication ELEC 3908, Physical Electronics, Lecture 15 Lecture Outline Now move on to bipolar junction transistor (BJT) Strategy for next few lectures similar to diode: structure and processing, basic operation,

More information

2. Nanoparticles. Introduction to Nanoscience, 2005 1

2. Nanoparticles. Introduction to Nanoscience, 2005 1 2. Nanoparticles Nanoparticles are the simplest form of structures with sizes in the nm range. In principle any collection of atoms bonded together with a structural radius of < 100 nm can be considered

More information

Molecular Beam Epitaxy

Molecular Beam Epitaxy Molecular Beam Epitaxy Klaus Ploog Paul Drude Institut Tutorial Session #1 Epitaxial Growth 27 th International Conference on the Physics of Semiconductors Flagstaff, AZ, 2004 Molecular Beam Epitaxy (MBE)

More information

Structure and properties of transparent conductive ZnO films grown by pulsed laser

Structure and properties of transparent conductive ZnO films grown by pulsed laser Structure and properties of transparent conductive ZnO films grown by pulsed laser deposition (PLD) by Yu Hsiu, Lin A dissertation submitted to the University of Birmingham for the degree of Master of

More information

Contamination. Cleanroom. Cleanroom for micro and nano fabrication. Particle Contamination and Yield in Semiconductors.

Contamination. Cleanroom. Cleanroom for micro and nano fabrication. Particle Contamination and Yield in Semiconductors. Fe Particles Metallic contaminants Organic contaminants Surface roughness Au Particles SiO 2 or other thin films Contamination Na Cu Photoresist Interconnect Metal N, P Damages: Oxide breakdown, metal

More information

Basics of LED drivers. Functions Requirements Selection

Basics of LED drivers. Functions Requirements Selection Andreas Hagemeyer Master of Science 05.2015 This article is meant to provide the reader with basic knowledge about the functional principle of LED luminaires, to explain the requirements for an LED driver

More information

MEMS mirror for low cost laser scanners. Ulrich Hofmann

MEMS mirror for low cost laser scanners. Ulrich Hofmann MEMS mirror for low cost laser scanners Ulrich Hofmann Outline Introduction Optical concept of the LIDAR laser scanner MEMS mirror requirements MEMS mirror concept, simulation and design fabrication process

More information

Steps to the exploitation of millimeter and sub-millimeter wave generation and detection for communication, sensing, and imaging

Steps to the exploitation of millimeter and sub-millimeter wave generation and detection for communication, sensing, and imaging Steps to the exploitation of millimeter and sub-millimeter wave generation and detection for communication, sensing, and imaging Collaboration: Germany: TU Darmstadt, Institut für Hochfrequenztechnik,

More information

Simultaneous data fitting in ARXPS

Simultaneous data fitting in ARXPS NOTE Please find the following more updated document Resolving overlapping peaks in ARXPS data: The effect of noise and fitting method. J. Muñoz-Flores, A. Herrera-Gomez, J. Electron Spectrosc. Relat.

More information

. Tutorial #3 Building Complex Targets

. Tutorial #3 Building Complex Targets . Tutorial #3 Building Complex Targets. Mixed Gas/Solid Targets Gas Ionization Chamber Previous Tutorials have covered how to setup TRIM, determine which ion and energy to specify for a semiconductor n-well

More information

SUPERCONDUCTIVITY. PH 318- Introduction to superconductors 1

SUPERCONDUCTIVITY. PH 318- Introduction to superconductors 1 SUPERCONDUCTIVITY property of complete disappearance of electrical resistance in solids when they are cooled below a characteristic temperature. This temperature is called transition temperature or critical

More information

Photonic components for signal routing in optical networks on chip

Photonic components for signal routing in optical networks on chip 15 th International Conference on Transparent Optical Networks Cartagena, Spain, June 23-27, 213 Photonic components for signal routing in optical networks on chip Vincenzo Petruzzelli, Giovanna Calò Dipartimento

More information

To meet the requirements of demanding new

To meet the requirements of demanding new Optimising LED manufacturing LED manufacturers seek new methods to reduce manufacturing costs and improve productivity in an increasingly demanding market. Tom Pierson, Ranju Arya, Columbine Robinson of

More information