Epitaxy is the deposition of layers, which are monocrystalline in large regions

Size: px
Start display at page:

Download "Epitaxy is the deposition of layers, which are monocrystalline in large regions"

Transcription

1 Repetition: Epitaxy Epitaxy is the deposition of layers, which are monocrystalline in large regions Homoepitaxy: Substrate material = film material Heteroepitaxy: Substrate material film material

2 Repetition: Heteroepitaxy I Epitactic relation: Substrate material Film material Van-der-Waals epitaxy: The interaction between substrate material and film material is so weak, that film atoms can arrange themselves in a crystallographically favorable manner.

3 Repetition: Heteroepitaxy II High temperature epitaxy: The crystallographically favorable arrangement of the atoms is reached by a high substrate temperature. Low temperature epitaxy : The crystallographically favorable arrangement of the atoms is reached by local defect structures Vicinal surfaces Dendritic Islands

4 Repetition: Growth Modes Growth modes: A: Substrate material B: Film material Frank-Van der Merwe: layer by layer W AB>WBB Volmer-Weber: islands, W AB<WBB Stranski-Krastanov: layer/island, W AB>WBB stress relief by 3d islands While the Frank-van der Merwe and Volmer-Weber Growth modes lead to mostly stress free films, in the Stranski-Krastanov-mode significant stresses are induced in the first growth phases.

5 Repetition: Stress/Film Growth Detailed mechanism: Lattice Mismatch : a a b 100[%] b Film, lattice constant b Pseudomorphic transition zone Substrate, lattice constant a a

6 Repetition: Roughness Types h(x) h max h min x Stochastic roughness h(x) a R R' R'' h Self similarity h(x) L L' R=f(L), R''>R'>R L'' x Ballistisc aggregate x

7 Repetition: Shadowing Peaks grow faster than valleys + Formation of columnar structures (a) + Pore formation in combination with surface diffusion (b) (a) (b)

8 Repetition: Roughness Values R a -value: mean absolute deviation R 1 N h a N h i i1 R q - or RMS-value: mean quadratic deviation R q R RMS RMS 1 N N h h i i1 2

9 Repetition: Correlation Functions Non normalized quantities Autocovariance function Normalized quantities Autocorrelation function R( ) h(x) h(x ) dx ( ) R( ) / R(0) Structure function S( ) [h(x) h(x )] 2 S( ) 2R 2 q [1 ( )] Note: All heigth values are measured from the mean heigth h.

10 Repetition: Correlation Length Surface profile Autocovariance function Within the profile exhibits similar heigth values. Periodicities are present, if R() exhibits maxima at 0.

11 Film Structure and Film Properties The film structure influences: + Density + Mechanical properties + Electric properties + Magnetic properties + Electronic properties

12 Application Profiles Depending on the application a certain film structure can be advantageous or disadvantageous: + Tool dense, fine grained + Biolog. material porous, soft + Elektronics dense, monocrystalline + Therm. barriers porous, hard

13 Structure Zone Models Growth phases of a coating Nucleation on substrate Partial coalescence and interface formation Total coalescence and polycrystal formation Growth of polycrystal grains Structure zone models yield a qualitative image of film growth, morphology and crystallography in dependence on the coating parameters.

14 Movchan-Demchishin: Evaporation

15 Thornton: Sputtering

16 Ion Plating

17 Zones and Growth Mechanisms Zone Mechanism Char. feature 1: T/T M <0,2 T: T/T M <0,4 2: T/T M <0,8 3: T/T M >0,8 Shadowing Particle energy Surface diffusion Volume diffusion Fibers, pores Nano grains Columnar crystlites 3d - Grains

18 Stresses Kinds of stresses: MECH T I Mechanical stress: MECH Thermal stress: T E S ( S U )(T B E S... Elastic modulus film S... CTE film U... CTE substrate T B... Deposition temperature T M... Measurement temperature T M ) Generated by clamping of the substrate and subsequent unclamping Generated by the different coefficients of Thermal Expansion (CTE) of substrate and coating

19 Stresses and Film Structure Intrinsic stress: I Intrinsic stresses are a direct consequence of the film structure and of the deposition conditions. Tensile stress Compressive stress Variable Compressive stress Tensile stress

20 Intrinsic Stresses: Sputtering

21 Stress Measurement: Fundamentals Curved substrate: Tensile stress Compressive stress Total stress of a thin film: Esd 6(1 2 s s )d F 1 R s1 1 R s2 a) Substrate b) Film c) Reference platelet E S... Elastic modulus substrate S... Poisson-number substrate d S... Thickness of substrate d F... Film thickness R S1, R S2... Radius of curvature before and after coating, respectively

22 Stress Measurement: Cantilever Geometry: Principle: tan(2) H Substrate Film Compressive stress Tensile stress l l R S 1 a tan 2 H l sin R S R S l 2 a tan H 2lH H Neglections and prerequisites: a) lateral displacement of the cantilever b) vertical displacement of the cantilever () c) low ratios /H

23 Stresses and Film Growth I In-Situ-measurements by the cantilever method: Tensile stress t COATING Type I: T large, mobility small M Compressive stress 0 Coalescence Type II: T small, mobility large M t Volume reduction by recrystallization after coating leads to tensile stresses Influence of the film thickness on I

24 Stresses and Film Growth II In-Situ-measurements by the cantilever method : Evaporation of Al -6 >10 mbar Type I Tensile stress 0 Compressive stress -11 <10 mbar mbar mbar t Type II Transition: segregation Influence of impurities in the residual gas During the evaporation process on I

25 Lattice Mismatch and Self Organization I Detailed mechanism: Lattice Mismatch : a a b 100[%] b Film, lattice constant b Pseudomorphic transition zone Substrate, lattice constant a a

26 Lattice Mismatch and Self Organization II Example: self organization of island positions in InAs/GaAs Multilayers: Quantum dot Interlayer Stranski-Krastanov wetting layer The lattice strain in the interlayer generates a preferred nucleation position directly above an island.

27 Stress Measurement by X-Rays Principle: Measurement of the global strain of the elementary cell generated by: + Interstitial atoms + Impurities Advantages: + Non-destructive + In Situ possible Disadvantages: Several other influences: + Lattice defects + Dislocations + Impurities + Foreign phases

28 Example: Temperature Variation Roentgenographic stress determination at variable temperature: Stress [MPa] Tensile stress Compressive stress as deposited Delamination 1. cycle: heating 1. cycle: cooling 2. cycle: heating 2. cycle: cooling Temperature [ C] Carbon substrate coated with 4 µm Cu Cu = 16 ppm/k C = 2 ppm/k

Repetition: Adhesion Mechanisms

Repetition: Adhesion Mechanisms Repetition: Adhesion Mechanisms a) Mechanical interlocking b) Monolayer/monolayer c) Chemical bonding d) Diffusion e) Psedo diffusion due to augmented energy input (hyperthermal particles) Repetition:

More information

Nucleation and growth of nanostructures and films. Seongshik (Sean) Oh

Nucleation and growth of nanostructures and films. Seongshik (Sean) Oh Nucleation and growth of nanostructures and films Seongshik (Sean) Oh Outline Introduction and Overview 1. Thermodynamics and Kinetics of thin film growth 2. Defects in films 3. Amorphous, Polycrystalline

More information

Applications for HFETs

Applications for HFETs Applications for HFETs Ga-face Quantum well is formed at the interface AlGaN GaN Buffer P SP P SP P PE -σ s +σ int 2DEG + ve φ b d σ comp AlGaN σ int E 0 GaN E c E F c-plane sapphire σ 2DEG σ surf Higher

More information

Previous Lecture. Vacuum & Plasma systems for. Dry etching

Previous Lecture. Vacuum & Plasma systems for. Dry etching Previous Lecture Vacuum & Plasma systems for Dry etching Lecture 9: Evaporation & sputtering Objectives From this evaporation lecture you will learn: Evaporator system layout & parts Vapor pressure Crucible

More information

X-ray optical thin film deposition and analysis capability at NASA MSFC. D. Broadway. 11/8/2017 D. Broadway NASA MSFC 1

X-ray optical thin film deposition and analysis capability at NASA MSFC. D. Broadway. 11/8/2017 D. Broadway NASA MSFC 1 X-ray optical thin film deposition and analysis capability at ASA MSFC D. Broadway /8/7 D. Broadway ASA MSFC Talk Outline Optical thin film coating capability at MSFC Deposition system X-ray reflectometer

More information

Lecture contents. Heteroepitaxy Growth technologies Strain Misfit dislocations. NNSE 618 Lecture #24

Lecture contents. Heteroepitaxy Growth technologies Strain Misfit dislocations. NNSE 618 Lecture #24 1 Lecture contents Heteroepitaxy Growth technologies Strain Misfit dislocations Epitaxy Heteroepitaxy 2 Single crystalline layer on Single crystalline substrate Strong layer-substrate interaction orientation

More information

Co-Evolution of Stress and Structure During Growth of Polycrystalline Thin Films

Co-Evolution of Stress and Structure During Growth of Polycrystalline Thin Films Co-Evolution of Stress and Structure During Growth of Polycrystalline Thin Films Carl V. Thompson and Hang Z. Yu* Dept. of Materials Science and Engineering MIT, Cambridge, MA, USA Effects of intrinsic

More information

CHAPTER 5 EFFECT OF POST DEPOSITION ANNEALING ON THE SURFACE MORPHOLOGY OF THE DLC FILM

CHAPTER 5 EFFECT OF POST DEPOSITION ANNEALING ON THE SURFACE MORPHOLOGY OF THE DLC FILM 86 CHAPTER 5 EFFECT OF POST DEPOSITION ANNEALING ON THE SURFACE MORPHOLOGY OF THE DLC FILM 5.1 INTRODUCTION Among various amorphous carbon films, DLC films produced via RF-PECVD have been successfully

More information

Ge/Si quantum dots and nanostructures

Ge/Si quantum dots and nanostructures Ge/Si quantum dots and nanostructures Nunzio Motta INFM-Università di Roma TRE Dr.Anna Sgarlata, Dr. M.Scarselli Prof. A.Balzarotti, Coworkers INFM-Dip. Fisica, Università di Roma Tor Vergata M.Scarselli

More information

Effects of Lead on Tin Whisker Elimination

Effects of Lead on Tin Whisker Elimination Effects of Lead on Tin Whisker Elimination Wan Zhang and Felix Schwager Rohm and Haas Electronic Materials Lucerne, Switzerland inemi Tin Whisker Workshop at ECTC 0 May 30, 2006, in San Diego, CA Efforts

More information

Chapter 2. Historical Perspective

Chapter 2. Historical Perspective 5 Chapter 2 Historical Perspective Physical vapor deposition generally refers to the growth of materials by the condensation of their vapor [26]. The vapor can be created by either thermal evaporation

More information

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

Lecture 12. Physical Vapor Deposition: Evaporation and Sputtering Reading: Chapter 12. ECE 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

Chapter 8: Strain Hardening and Annealing

Chapter 8: Strain Hardening and Annealing Slide 1 Chapter 8: Strain Hardening and Annealing 8-1 Slide 2 Learning Objectives 1. Relationship of cold working to the stress-strain curve 2. Strain-hardening mechanisms 3. Properties versus percent

More information

Institute of Solid State Physics. Technische Universität Graz. Deposition. Franssila: Chapters 5 & 6. Peter Hadley

Institute of Solid State Physics. Technische Universität Graz. Deposition. Franssila: Chapters 5 & 6. Peter Hadley Technische Universität Graz Institute of Solid State Physics Deposition Franssila: Chapters 5 & 6 Peter Hadley Silicon wafers Total Thickness Variation: a good 8" Prime wafer would be < 15 m Site flatness

More information

"Thin Film Technology" "Physics of Thin Films"

Thin Film Technology Physics of Thin Films D r d "Thin Film Technology" "Physics of Thin Films" Contents: Preface 1. Introduction 1.1. General 1.2. History 1.3. Definition of Terms 1.4. Applications of Thin Film Technology 1.5. Deposition Methods

More information

8. Epitaxy. - Extended single-crystal film formation on top of a crystalline substrate

8. Epitaxy. - Extended single-crystal film formation on top of a crystalline substrate 8. Epitaxy 1. Introduction επι(epi placed or resting upon) ταξιζ(taxis arrangement) - Extended single-crystal film formation on top of a crystalline substrate - Homoepitaxy : Film and substrate are the

More information

Learning Objectives. Chapter Outline. Solidification of Metals. Solidification of Metals

Learning Objectives. Chapter Outline. Solidification of Metals. Solidification of Metals Learning Objectives Study the principles of solidification as they apply to pure metals. Examine the mechanisms by which solidification occurs. - Chapter Outline Importance of Solidification Nucleation

More information

Micro-Electro-Mechanical Systems (MEMS) Fabrication. Special Process Modules for MEMS. Principle of Sensing and Actuation

Micro-Electro-Mechanical Systems (MEMS) Fabrication. Special Process Modules for MEMS. Principle of Sensing and Actuation Micro-Electro-Mechanical Systems (MEMS) Fabrication Fabrication Considerations Stress-Strain, Thin-film Stress, Stiction Special Process Modules for MEMS Bonding, Cavity Sealing, Deep RIE, Spatial forming

More information

STRENGTHENING MECHANISM IN METALS

STRENGTHENING MECHANISM IN METALS Background Knowledge Yield Strength STRENGTHENING MECHANISM IN METALS Metals yield when dislocations start to move (slip). Yield means permanently change shape. Slip Systems Slip plane: the plane on which

More information

Deposition and characterization of sputtered ZnO films

Deposition and characterization of sputtered ZnO films Superlattices and Microstructures 42 (2007) 89 93 www.elsevier.com/locate/superlattices Deposition and characterization of sputtered ZnO films W.L. Dang, Y.Q. Fu, J.K. Luo, A.J. Flewitt, W.I. Milne Electrical

More information

Micro-Electro-Mechanical Systems (MEMS) Fabrication. Special Process Modules for MEMS. Principle of Sensing and Actuation

Micro-Electro-Mechanical Systems (MEMS) Fabrication. Special Process Modules for MEMS. Principle of Sensing and Actuation Micro-Electro-Mechanical Systems (MEMS) Fabrication Fabrication Considerations Stress-Strain, Thin-film Stress, Stiction Special Process Modules for MEMS Bonding, Cavity Sealing, Deep RIE, Spatial forming

More information

Improving the Performance of Ceramic Barrier Layers used in Packaging Materials

Improving the Performance of Ceramic Barrier Layers used in Packaging Materials Improving the Performance of Ceramic Barrier Layers used in Packaging Materials Roland Trassl Senior Manager Advanced Development Applied Materials WEB Coating GmbH AIMCAL Tampa, Florida, USA 18 th October,

More information

Nuclear Fuel Engineering (2. Modeling) Department of Nuclear Eng. KHU Kwnagheon Park

Nuclear Fuel Engineering (2. Modeling) Department of Nuclear Eng. KHU Kwnagheon Park Nuclear Fuel Engineering (2. Modeling) Department of Nuclear Eng. KHU Kwnagheon Park 2. Behaviors of Pellet during Normal Operation 2 2.1. Temperature Distribution in a Fuel Rod C p T t kt q ''' ( r) Macroscopic

More information

InGaN quantum dot based LED for white light emitting

InGaN quantum dot based LED for white light emitting Emerging Photonics 2014 InGaN quantum dot based LED for white light emitting Luo Yi, Wang Lai, Hao Zhibiao, Han Yanjun, and Li Hongtao Tsinghua National Laboratory for Information Science and Technology,

More information

much research (in physics, chemistry, material science, etc.) have been done to understand the difference in materials properties.

much research (in physics, chemistry, material science, etc.) have been done to understand the difference in materials properties. 1.1: Introduction Material science and engineering Classify common features of structure and properties of different materials in a well-known manner (chemical or biological): * bonding in solids are classified

More information

2008 Summer School on Spin Transfer Torque

2008 Summer School on Spin Transfer Torque 2008 Summer School on Spin Transfer Torque Nano-scale device fabrication 2-July-2008 Byoung-Chul Min Center for Spintronics Research Korea Institute of Science and Technology Introduction Moore s Law

More information

Investigation and growth of nickel coatings for electrical contact applications

Investigation and growth of nickel coatings for electrical contact applications IFM, Department of Physics, Chemistry and Biology. Master s thesis Investigation and growth of nickel coatings for electrical contact applications Maria Fawakhiri LITH-IFM-A-EX--09/2059 SE IFM Department

More information

Thin Film Scattering: Epitaxial Layers

Thin Film Scattering: Epitaxial Layers Thin Film Scattering: Epitaxial Layers 6th Annual SSRL Workshop on Synchrotron X-ray Scattering Techniques in Materials and Environmental Sciences: Theory and Application May 29-31, 2012 Thin films. Epitaxial

More information

Materials Science and Engineering: An Introduction

Materials Science and Engineering: An Introduction Materials Science and Engineering: An Introduction Callister, William D. ISBN-13: 9780470419977 Table of Contents List of Symbols. 1 Introduction. 1.1 Historical Perspective. 1.2 Materials Science and

More information

RBS AND NRS ANALYSIS OF SPUTTERED NB FILMS ANNEALED AT DIFFERENT TEMPERATURES

RBS AND NRS ANALYSIS OF SPUTTERED NB FILMS ANNEALED AT DIFFERENT TEMPERATURES RBS AND NRS ANALYSIS OF SPUTTERED NB FILMS ANNEALED AT DIFFERENT TEMPERATURES M.RIBEAUDEAU, P.BOSLAND Service d'etude des Accélérateurs, CEA/SACLAY, F-91 191 Gif-sur-Yvette A.CHEVARIER, O.GUISE, P.TROUVE

More information

1. Introduction. What is implantation? Advantages

1. Introduction. What is implantation? Advantages Ion implantation Contents 1. Introduction 2. Ion range 3. implantation profiles 4. ion channeling 5. ion implantation-induced damage 6. annealing behavior of the damage 7. process consideration 8. comparison

More information

Ferromagnetic transition in Ge 1 x Mn x Te semiconductor layers

Ferromagnetic transition in Ge 1 x Mn x Te semiconductor layers Materials Science-Poland, Vol. 25, No. 2, 2007 Ferromagnetic transition in Ge 1 x Mn x Te semiconductor layers W. KNOFF *, P. DZIAWA, V. OSINNIY, B. TALIASHVILI, V. DOMUCHOWSKI, E. ŁUSAKOWSKA, K. ŚWIĄTEK,

More information

High Anisotropy L1 0 FePt Media for Perpendicular Magnetic Recording Applications

High Anisotropy L1 0 FePt Media for Perpendicular Magnetic Recording Applications DISKCON 2008 High Anisotropy L1 0 FePt Media for Perpendicular Magnetic Recording Applications Boon Chow LIM Agency for Science Technology & Research (A*STAR) DATA STORAGE INSTITUTE 5 Engineering Drive

More information

Ultra High Barrier Coatings by PECVD

Ultra High Barrier Coatings by PECVD Society of Vacuum Coaters 2014 Technical Conference Presentation Ultra High Barrier Coatings by PECVD John Madocks & Phong Ngo, General Plasma Inc., 546 E. 25 th Street, Tucson, Arizona, USA Abstract Silicon

More information

Understanding residual stress in polycrystalline thin films through real-time. measurements and physical models. Eric Chason and Pradeep R.

Understanding residual stress in polycrystalline thin films through real-time. measurements and physical models. Eric Chason and Pradeep R. Understanding residual stress in polycrystalline thin films through real-time measurements and physical models Eric Chason and Pradeep R. Guduru School of Engineering Brown University, Providence, RI Abstract

More information

Fracture. Brittle vs. Ductile Fracture Ductile materials more plastic deformation and energy absorption (toughness) before fracture.

Fracture. Brittle vs. Ductile Fracture Ductile materials more plastic deformation and energy absorption (toughness) before fracture. 1- Fracture Fracture: Separation of a body into pieces due to stress, at temperatures below the melting point. Steps in fracture: 1-Crack formation 2-Crack propagation There are two modes of fracture depending

More information

Potential of High Velocity Oxy Fuel Thermal Spraying in Turbine Shaft Repairing. Production Technology Research Institute, branch of ACECR

Potential of High Velocity Oxy Fuel Thermal Spraying in Turbine Shaft Repairing. Production Technology Research Institute, branch of ACECR Potential of High Velocity Oxy Fuel Thermal Spraying in Turbine Shaft Repairing M. Jalali Azizpour 1 S. Norouzi H.Mohammadi Majd 3 D.Sajedipour 4 E. Pipelzadeh 5 B.Aslani 6 H.Talebi 7 A.Ghamari 8 1, 3,

More information

The effect of ion milling on the morphology of ramp-type Josephson junctions

The effect of ion milling on the morphology of ramp-type Josephson junctions Journal of MATERIALS RESEARCH Welcome Comments Help The effect of ion milling on the morphology of ramp-type Josephson junctions Dave H. A. Blank and Horst Rogalla Low Temperature Division, Department

More information

CHAPTER 8 CONCLUSIONS AND SUGGESTIONS FOR FUTURE WORK

CHAPTER 8 CONCLUSIONS AND SUGGESTIONS FOR FUTURE WORK CHAPTER 8 CONCLUSIONS AND SUGGESTIONS FOR FUTURE WORK 8.1. Conclusions Referring to the aims of the research project in Chapter 4, the following conclusions can be drawn on the basis of the present work:

More information

Formation mechanism of new corrosion resistance magnesium thin films by PVD method

Formation mechanism of new corrosion resistance magnesium thin films by PVD method Surface and Coatings Technology 169 170 (2003) 670 674 Formation mechanism of new corrosion resistance magnesium thin films by PVD method a, a a a b M.H. Lee *, I.Y. Bae, K.J. Kim, K.M. Moon, T. Oki a

More information

to which it is applied. Using this approach temperature drops of up to 170 o C at the metal

to which it is applied. Using this approach temperature drops of up to 170 o C at the metal Chapter 2 Thermal Barrier Coatings 2.1 Overview By attaching an adherent layer of a low thermal conductivity material to the surface of a internally cooled gas turbine blade, a temperature drop can be

More information

EPITAXY extended single-crystal film formation on top of a crystalline substrate. Homoepitaxy (Si on Si) Heteroepitaxy (AlAs on GaAs)

EPITAXY extended single-crystal film formation on top of a crystalline substrate. Homoepitaxy (Si on Si) Heteroepitaxy (AlAs on GaAs) extended single-crystal film formation on top of a crystalline substrate Homoepitaxy (Si on Si) Heteroepitaxy (AlAs on GaAs) optoelectronic devices (GaInN) high-frequency wireless communication devices

More information

OUTLINE. Preparation of III Nitride thin 6/10/2010

OUTLINE. Preparation of III Nitride thin 6/10/2010 Preparation of III Nitride thin films for LEDs Huaxiang Shen Supervisor: Dr. Adrian Kitai 1 2 Two kinds of EL devices Light emitting diodes Powder EL and thin film EL http://en.wikipedia.org/wiki/file:pnjunction

More information

Keywords: Porous III-V semiconductors, Electrochemical etching, Pore conversion, Heteroepitaxial growth.

Keywords: Porous III-V semiconductors, Electrochemical etching, Pore conversion, Heteroepitaxial growth. APPLICATIONS OF POROUS III-V SEMICONDUCTORS IN HETEROEPITAXIAL GROWTH AND IN THE PREPARATION OF NANOCOMPOSITE STRUCTURES Dušan NOHAVICA a,b, Jan GRYM a, Petar GLADKOV a,b, Eduard HULICIUS b, Jiří PANGRAC

More information

Annealing Effect on Elastic Constant of Ultrathin Films Studied by Acoustic-Phonon Resonance Spectroscopy

Annealing Effect on Elastic Constant of Ultrathin Films Studied by Acoustic-Phonon Resonance Spectroscopy 1st International Symposium on Laser Ultrasonics: Science, Technology and Applications July 16-18 28, Montreal, Canada Annealing Effect on Elastic Constant of Ultrathin Films Studied by Acoustic-Phonon

More information

In situ TEM Characterization of Shear Stress-Induced Interlayer. Sliding in the Cross Section View of Molybdenum Disulfide

In situ TEM Characterization of Shear Stress-Induced Interlayer. Sliding in the Cross Section View of Molybdenum Disulfide In situ TEM Characterization of Shear Stress-Induced Interlayer Sliding in the Cross Section View of Molybdenum Disulfide Juan Pablo Oviedo, Santosh KC, Ning Lu, Jinguo Wang, Kyeongjae Cho, Robert M. Wallace,

More information

Synthesis of nanoscale CN x /TiAlN multilayered coatings by ion-beam-assisted deposition

Synthesis of nanoscale CN x /TiAlN multilayered coatings by ion-beam-assisted deposition Synthesis of nanoscale / multilayered coatings by ion-beam-assisted deposition M. Cao, D. J. Li, a and X. Y. Deng College of Physics and Electronic Information Science, Tianjin Normal University, Tianjin

More information

Metallization deposition and etching. Material mainly taken from Campbell, UCCS

Metallization deposition and etching. Material mainly taken from Campbell, UCCS Metallization deposition and etching Material mainly taken from Campbell, UCCS Application Metallization is back-end processing Metals used are aluminum and copper Mainly involves deposition and etching,

More information

Ultrathin Metal Films

Ultrathin Metal Films Matthias Wuttig Xiangdong Liu Ultrathin Metal Films Magnetic and Structural Properties With 234 Figures 4u Springer Contents 1 Introduction 1 References 4 2 Growth of Ultrathin Metal Films 5 2.1 Growth

More information

Development of High Throughput CIGS Manufacturing Process. PI: Neelkanth Dhere Students: Sachin Kulkarni, Ph.D.; Ph.D.; Ashwani Kaul, Ph.D.

Development of High Throughput CIGS Manufacturing Process. PI: Neelkanth Dhere Students: Sachin Kulkarni, Ph.D.; Ph.D.; Ashwani Kaul, Ph.D. UNIVERSITY OF CENTRAL FLORIDA Development of High Throughput CIGS Manufacturing Process PI: Neelkanth Dhere Students: Sachin Kulkarni, Ph.D.; Ph.D.; Ashwani Kaul, Ph.D. Description: A reduction in the

More information

Fabrication of Highly Ordered Al 2 O 3 Nanohole Arrays As a Nanostructured Template

Fabrication of Highly Ordered Al 2 O 3 Nanohole Arrays As a Nanostructured Template Fabrication of Highly Ordered Al 2 O 3 Nanohole Arrays As a Nanostructured Template Jie Gong, Bill Butler and Giovanni Zangari Materials Science Program University of Alabama at Tuscaloosa This work was

More information

NASF SURFACE TECHNOLOGY WHITE PAPERS 81 (5), (May 2017) 4 th Quarterly Report October-December 2016 AESF Research Project #R-118

NASF SURFACE TECHNOLOGY WHITE PAPERS 81 (5), (May 2017) 4 th Quarterly Report October-December 2016 AESF Research Project #R-118 4 th Quarterly Report October-December 2016 AESF Research Project #R-118 Crack Formation during Electrodeposition and Post-deposition Aging of Thin Film Coatings by Prof. Stanko R. Brankovic * University

More information

Thin Film Scattering: Epitaxial Layers

Thin Film Scattering: Epitaxial Layers Thin Film Scattering: Epitaxial Layers Arturas Vailionis First Annual SSRL Workshop on Synchrotron X-ray Scattering Techniques in Materials and Environmental Sciences: Theory and Application Tuesday, May

More information

Vertical nano-composite heteroepitaxial thin films with manganites and ferroelectrics. Yonghang Pei Physics Department

Vertical nano-composite heteroepitaxial thin films with manganites and ferroelectrics. Yonghang Pei Physics Department Vertical nano-composite heteroepitaxial thin films with manganites and ferroelectrics Yonghang Pei Physics Department Outline Introduction to MultiFerroics La 1 x Sr x MnO 3 Experiment Summary and Future

More information

FINITE ELEMENT ANALYSIS OF THE BONDCOAT INFLUENCE ON RESIDUAL STRESS DURING THE PLASMA THERMAL SPRAYING OF PARTIALLY STABILISED ZIRCONIA

FINITE ELEMENT ANALYSIS OF THE BONDCOAT INFLUENCE ON RESIDUAL STRESS DURING THE PLASMA THERMAL SPRAYING OF PARTIALLY STABILISED ZIRCONIA FINITE ELEMENT ANALYSIS OF THE BONDCOAT INFLUENCE ON RESIDUAL STRESS DURING THE PLASMA THERMAL SPRAYING OF PARTIALLY STABILISED ZIRCONIA P. Fogarassy (1,2), F. Rotaru (1), N. Markocsan (1), B.B. Straumal

More information

AN INVESTIGATION OF DIAMOND THIN FILM DEPOSITION ON STEEL SUBSTRATES

AN INVESTIGATION OF DIAMOND THIN FILM DEPOSITION ON STEEL SUBSTRATES AN INVESTIGATION OF DIAMOND THIN FILM DEPOSITION ON STEEL SUBSTRATES VOJTĚCH KUNDRÁT Doctor of Philosophy ASTON UNIVERSITY October 2015 Vojtěch Kundrát, 2015 This copy of thesis has been supplied on condition

More information

Development of New Generation Of Coatings with Strength-Ductility Relationship, Wear, Corrosion and Hydrogen Embrittlement Resistance Beyond the

Development of New Generation Of Coatings with Strength-Ductility Relationship, Wear, Corrosion and Hydrogen Embrittlement Resistance Beyond the Development of New Generation Of Coatings with Strength-Ductility Relationship, Wear, Corrosion and Hydrogen Embrittlement Resistance Beyond the Current Materials Accomplishments till date As the structural

More information

CHAPTER 3. Experimental Results of Magnesium oxide (MgO) Thin Films

CHAPTER 3. Experimental Results of Magnesium oxide (MgO) Thin Films CHAPTER 3 Experimental Results of Magnesium oxide (MgO) Thin Films Chapter: III ---------------------------------------------------------------- Experimental Results of Magnesium oxide (MgO) Thin Films

More information

SUPER HARDENING OF W/NbN NANOLAYERS UNDER SHALLOW NANOINDENTATION. Brian Michael Ennis. BSME, University of Pittsburgh, 2002

SUPER HARDENING OF W/NbN NANOLAYERS UNDER SHALLOW NANOINDENTATION. Brian Michael Ennis. BSME, University of Pittsburgh, 2002 SUPER HARDENING OF W/NbN NANOLAYERS UNDER SHALLOW NANOINDENTATION by Brian Michael Ennis BSME, University of Pittsburgh, 2002 Submitted to the Graduate Faculty of School of Engineering in partial fulfillment

More information

SIMULATION OF THE DEPOSITION OF BCC METALS INCLUDING ANISTROPIC EFFECTS USING 3D-Films

SIMULATION OF THE DEPOSITION OF BCC METALS INCLUDING ANISTROPIC EFFECTS USING 3D-Films SIMULATION OF THE DEPOSITION OF BCC METALS INCLUDING ANISTROPIC EFFECTS USING 3D-Films T. Smy and R.V. Joshi 1 Dept. of Electronics, Carleton University, Ottawa, ON, Canada K1S 5B6, ph: 613-520-3967, fax:

More information

Lecture Day 2 Deposition

Lecture Day 2 Deposition Deposition Lecture Day 2 Deposition PVD - Physical Vapor Deposition E-beam Evaporation Thermal Evaporation (wire feed vs boat) Sputtering CVD - Chemical Vapor Deposition PECVD LPCVD MVD ALD MBE Plating

More information

Chapter Outline: Failure

Chapter Outline: Failure Chapter Outline: Failure How do Materials Break? Ductile vs. brittle fracture Principles of fracture mechanics Stress concentration Impact fracture testing Fatigue (cyclic stresses) Cyclic stresses, the

More information

Through Silicon Vias Annealing: A thermo-mechanical assessment

Through Silicon Vias Annealing: A thermo-mechanical assessment Dresden University of Technology / Through Silicon Vias Annealing: P. Saettler (1), K. J. Wolter (1), M. Hecker (2), M. Boettcher (3) and C. Rudolph (3) (1) Technische Universität Dresden, (2) Globalfoundries

More information

The influence of the internal microstructure on the surface parameters of polycrystalline thin films

The influence of the internal microstructure on the surface parameters of polycrystalline thin films The influence of the internal microstructure on the surface parameters of polycrystalline thin films C. Eisenmenger-Sittner and A. Bergauer Institut für Angewandte und Technische Physik, Technische Universität

More information

Lecture 22: Integrated circuit fabrication

Lecture 22: Integrated circuit fabrication Lecture 22: Integrated circuit fabrication Contents 1 Introduction 1 2 Layering 4 3 Patterning 7 4 Doping 8 4.1 Thermal diffusion......................... 10 4.2 Ion implantation.........................

More information

Introduction to Engineering Materials ENGR2000 Chapter 7: Dislocations and Strengthening Mechanisms. Dr. Coates

Introduction to Engineering Materials ENGR2000 Chapter 7: Dislocations and Strengthening Mechanisms. Dr. Coates Introduction to Engineering Materials ENGR2000 Chapter 7: Dislocations and Strengthening Mechanisms Dr. Coates An edge dislocation moves in response to an applied shear stress dislocation motion 7.1 Introduction

More information

Measurement of Residual Stress by X-ray Diffraction

Measurement of Residual Stress by X-ray Diffraction Measurement of Residual Stress by X-ray Diffraction C-563 Overview Definitions Origin Methods of determination of residual stresses Method of X-ray diffraction (details) References End Stress and Strain

More information

NANO SCRATCH TESTING OF THIN FILM ON GLASS SUBSTRATE

NANO SCRATCH TESTING OF THIN FILM ON GLASS SUBSTRATE NANO SCRATCH TESTING OF THIN FILM ON GLASS SUBSTRATE Prepared by Jesse Angle 6 Morgan, Ste156, Irvine CA 92618 P: 949.461.9292 F: 949.461.9232 nanovea.com Today's standard for tomorrow's materials. 2010

More information

Problems to the lecture Physical Metallurgy ( Materialkunde ) Chapter 6: Mechanical Properties

Problems to the lecture Physical Metallurgy ( Materialkunde ) Chapter 6: Mechanical Properties Institut für Metallkunde und Metallphysik Direktor: Prof. Dr. rer. nat. Günter Gottstein RWTH Aachen, D-52056 Aachen Internet: http://www.imm.rwth-aachen.de E-mail: imm@imm.rwth-aachen.de Tel.: +49 241

More information

Structural changes of polycrystalline silicon layers during high temperature annealing

Structural changes of polycrystalline silicon layers during high temperature annealing Structural changes of polycrystalline silicon layers during high temperature annealing D. Lysáček, L. Válek ON SEMICONDUCTOR CZECH REPUBLIC, Rožnov p. R., david.lysacek@onsemi.com Abstract The structure

More information

X-RAY DIFFRACTION IN SEMICONDUCTOR INDUSTRY AND RESEARCH

X-RAY DIFFRACTION IN SEMICONDUCTOR INDUSTRY AND RESEARCH X-RAY DIFFRACTION IN SEMICONDUCTOR INDUSTRY AND RESEARCH M. Leszczyński High Pressure Research Center UNIPRESS, Sokolowska 29/37, 01 142 Warsaw, Poland, e-mail: mike@unipress.waw.pl ABSTRACT The paper

More information

Supplementary Figure S1 Crystal structure of the conducting filaments in sputtered SiO 2

Supplementary Figure S1 Crystal structure of the conducting filaments in sputtered SiO 2 Supplementary Figure S1 Crystal structure of the conducting filaments in sputtered SiO 2 based devices. (a) TEM image of the conducting filament in a SiO 2 based memory device used for SAED analysis. (b)

More information

HONEYCOMB MECHANICAL BEHAVIOR USING MACROINDENTATION

HONEYCOMB MECHANICAL BEHAVIOR USING MACROINDENTATION HONEYCOMB MECHANICAL BEHAVIOR USING MACROINDENTATION. Prepared by Duanjie Li, PhD 6 Morgan, Ste156, Irvine CA 92618 P: 949.461.9292 F: 949.461.9232 nanovea.com Today's standard for tomorrow's materials.

More information

ENCAPSULATION OF ORGANIC LIGHT EMITTING DIODES

ENCAPSULATION OF ORGANIC LIGHT EMITTING DIODES ENCAPSULATION OF ORGANIC LIGHT EMITTING DIODES Bhadri Visweswaran Sigurd Wagner, James Sturm, Electrical Engineering, Princeton University, NJ Siddharth Harikrishna Mohan, Prashant Mandlik, Jeff Silvernail,

More information

Three-dimensional epitaxy: Thermodynamic stability range of coherent germanium nanocrystallites in silicon

Three-dimensional epitaxy: Thermodynamic stability range of coherent germanium nanocrystallites in silicon Three-dimensional epitaxy: Thermodynamic stability range of coherent germanium nanocrystallites in silicon S. Balasubramanian, a) G. Ceder, and K. D. Kolenbrander Department of Materials Science and Engineering,

More information

Development of W Coatings for Fusion Applications

Development of W Coatings for Fusion Applications EFDA JET CP(10)07/26 C. Ruset, E. Grigore, H. Maier, R. Neu, H. Greuner, M. Mayer, G. Matthews and JET EFDA contributors Development of W Coatings for Fusion Applications This document is intended for

More information

Characterization and erosion of metal-containing carbon layers

Characterization and erosion of metal-containing carbon layers Characterization and erosion of metal-containing carbon layers Martin Balden Max-Planck-Institut für Plasmaphysik, EURATOM Association, D-85748 Garching, Germany Materials Research Division (MF) Outline

More information

Chapter 10, Phase Transformations

Chapter 10, Phase Transformations Chapter Outline: Phase Transformations Heat Treatment (time and temperature) Microstructure Kinetics of phase transformations Homogeneous and heterogeneous nucleation Growth, rate of the phase transformation

More information

Thermal Evaporation. Theory

Thermal Evaporation. Theory Thermal Evaporation Theory 1. Introduction Procedures for depositing films are a very important set of processes since all of the layers above the surface of the wafer must be deposited. We can classify

More information

Introduction to Materials Science

Introduction to Materials Science EPMA Powder Metallurgy Summer School 27 June 1 July 2016 Valencia, Spain Introduction to Materials Science Prof. Alberto Molinari University of Trento, Italy Some of the figures used in this presentation

More information

Specimen Preparation Technique for a Microstructure Analysis Using the Focused Ion Beam Process

Specimen Preparation Technique for a Microstructure Analysis Using the Focused Ion Beam Process Specimen Preparation Technique for a Microstructure Analysis Using the Focused Ion Beam Process by Kozue Yabusaki * and Hirokazu Sasaki * In recent years the FIB technique has been widely used for specimen

More information

Semiconductor Nanostructures

Semiconductor Nanostructures I H. von Känel Laboratorium für Festkörperphysik ETHZ Moore s Law Doubling of transistor density in less than every 2 years International Roadmap for Semiconductors Evolution of LED performance Haitz law

More information

ME 254 MATERIALS ENGINEERING 1 st Semester 1431/ rd Mid-Term Exam (1 hr)

ME 254 MATERIALS ENGINEERING 1 st Semester 1431/ rd Mid-Term Exam (1 hr) 1 st Semester 1431/1432 3 rd Mid-Term Exam (1 hr) Question 1 a) Answer the following: 1. Do all metals have the same slip system? Why or why not? 2. For each of edge, screw and mixed dislocations, cite

More information

Assume that the growth of fatigue cracks in the plate is governed by a Paris type of law, i.e. da

Assume that the growth of fatigue cracks in the plate is governed by a Paris type of law, i.e. da 3. Mechanical Properties of Materials Exam #3 May 16, 00 This examination contains 9 single-sided pages. Please give your answers only in this examination booklet. Do not use any other sheets of paper.

More information

INTERFACES AND STRESSES IN THIN FILMS p

INTERFACES AND STRESSES IN THIN FILMS p Acta mater. 48 (2000) 31±42 www.elsevier.com/locate/actamat INTERFACES AND STRESSES IN THIN FILMS p F. SPAEPEN Division of Engineering and Applied Sciences, Harvard University, Cambridge, MA 02138, USA

More information

Theory of Tin Whisker Growth The End Game. Joe Smetana inemi Tin Whisker Workshop at ECTC May 31, 2005

Theory of Tin Whisker Growth The End Game. Joe Smetana inemi Tin Whisker Workshop at ECTC May 31, 2005 Theory of Tin Whisker Growth The End Game Joe Smetana inemi Tin Whisker Workshop at ECTC May 31, 2005 Dislocation Theories Growth at the Tip History Growth Mechanisms 1952 Peach Dislocation Mechanism 1976

More information

Atomistic Mechanisms of Stress Evolution for Gold Thin Films on Nickel Substrates via Molecular Dynamics Simulations

Atomistic Mechanisms of Stress Evolution for Gold Thin Films on Nickel Substrates via Molecular Dynamics Simulations Lehigh University Lehigh Preserve Theses and Dissertations 2016 Atomistic Mechanisms of Stress Evolution for Gold Thin Films on Nickel Substrates via Molecular Dynamics Simulations Murat Al Lehigh University

More information

Doping and Oxidation

Doping and Oxidation Technische Universität Graz Institute of Solid State Physics Doping and Oxidation Franssila: Chapters 13,14, 15 Peter Hadley Technische Universität Graz Institute of Solid State Physics Doping Add donors

More information

Point Defects. Vacancies are the most important form. Vacancies Self-interstitials

Point Defects. Vacancies are the most important form. Vacancies Self-interstitials Grain Boundaries 1 Point Defects 2 Point Defects A Point Defect is a crystalline defect associated with one or, at most, several atomic sites. These are defects at a single atom position. Vacancies Self-interstitials

More information

Chapter 5: Atom and Ion Movements in Materials

Chapter 5: Atom and Ion Movements in Materials Slide 1 Chapter 5: Atom and Ion Movements in Materials 5-1 Slide 2 Learning Objectives 1. Applications of diffusion 2. Stability of atoms and ions 3. Mechanisms for diffusion 4. Activation energy for diffusion

More information

Available online at ScienceDirect. Procedia Engineering 79 (2014 )

Available online at  ScienceDirect. Procedia Engineering 79 (2014 ) Available online at www.sciencedirect.com ScienceDirect Procedia Engineering 79 (2014 ) 212 217 37th National Conference on Theoretical and Applied Mechanics (37th NCTAM 2013) & The 1st International Conference

More information

Magnetic patterning: local manipulation of the intergranular. exchange coupling via grain boundary engineering

Magnetic patterning: local manipulation of the intergranular. exchange coupling via grain boundary engineering Magnetic patterning: local manipulation of the intergranular exchange coupling via grain boundary engineering Kuo-Feng Huang, 1 Jung-Wei Liao, 1 Cheng-Yu Hsieh, 2 Liang-Wei Wang, 1 Yen-Chun Huang, 1 Wei-Chih

More information

Optically Assisted Metal-Induced Crystallization of Thin Si Films for Low-Cost Solar Cells

Optically Assisted Metal-Induced Crystallization of Thin Si Films for Low-Cost Solar Cells Optically Assisted Metal-Induced Crystallization of Thin Si Films for Low-Cost Solar Cells Wei Chen, Bhushan Sopori, Kim Jones, and Robert Reedy, National Renewable Energy Laboratory, Golden, CO; N. M.

More information

Research Article Properties of RF-Sputtered PZT Thin Films with Ti/Pt Electrodes

Research Article Properties of RF-Sputtered PZT Thin Films with Ti/Pt Electrodes International Polymer Science, Article ID 574684, 5 pages http://dx.doi.org/10.1155/2014/574684 Research Article Properties of RF-Sputtered PZT Thin Films with Ti/Pt Electrodes Cui Yan, Yao Minglei, Zhang

More information

IMRE/ETPL Flagship Project

IMRE/ETPL Flagship Project IMRE/ETPL Flagship Project Nanoparticulate Barrier Films & Gas Permeation Measurement Techniques for Thin Film Solar & Display Application Problems Senthil Ramadas Institute of Materials Research & Engineering

More information

3.46 OPTICAL AND OPTOELECTRONIC MATERIALS

3.46 OPTICAL AND OPTOELECTRONIC MATERIALS Badgap Engineering: Precise Control of Emission Wavelength Wavelength Division Multiplexing Fiber Transmission Window Optical Amplification Spectrum Design and Fabrication of emitters and detectors Composition

More information

Imperfections in the Atomic and Ionic Arrangements

Imperfections in the Atomic and Ionic Arrangements Objectives Introduce the three basic types of imperfections: point defects, line defects (or dislocations), and surface defects. Explore the nature and effects of different types of defects. Outline Point

More information

BONDING OF MULTIPLE WAFERS FOR HIGH THROUGHPUT LED PRODUCTION. S. Sood and A. Wong

BONDING OF MULTIPLE WAFERS FOR HIGH THROUGHPUT LED PRODUCTION. S. Sood and A. Wong 10.1149/1.2982882 The Electrochemical Society BONDING OF MULTIPLE WAFERS FOR HIGH THROUGHPUT LED PRODUCTION S. Sood and A. Wong Wafer Bonder Division, SUSS MicroTec Inc., 228 SUSS Drive, Waterbury Center,

More information

FePd (216 Å) grown on (001) MgO. 2θ(deg)

FePd (216 Å) grown on (001) MgO. 2θ(deg) Major Findings 1. FePd thin films The structural characterization of the films grown at various substrate temperatures (RT- 700 o C) was performed ex-situ using X-Ray Diffraction (XRD). The optimum substrate

More information

Micro-Electro-Mechanical Systems (MEMS) Fabrication. Special Process Modules for MEMS. Principle of Sensing and Actuation

Micro-Electro-Mechanical Systems (MEMS) Fabrication. Special Process Modules for MEMS. Principle of Sensing and Actuation Micro-Electro-Mechanical Systems (MEMS) Fabrication Fabrication Considerations Stress-Strain, Thin-film Stress, Stiction Special Process Modules for MEMS Bonding, Cavity Sealing, Deep RIE, Spatial forming

More information