Nova 600 NanoLab Dual beam Focused Ion Beam IITKanpur

Size: px
Start display at page:

Download "Nova 600 NanoLab Dual beam Focused Ion Beam IITKanpur"

Transcription

1 Nova 600 NanoLab Dual beam Focused Ion Beam IITKanpur Dual Beam Nova 600 Nano Lab From FEI company (Dual Beam = SEM + FIB) SEM: The Electron Beam for SEM Field Emission Electron Gun Energy : 500 ev to 30 kev Current : 0.7 pa to 37 na Beam spot size : 1.1 to 10 nm Magnification upto X FIB : The Ga Ion Beam for FIB modifications Ga liquid metal ion source (LMIS) Energy : 5 kev to 30 kev Current : 0.3 pa to 20 na Beam spot size : 7 to 15 nm Five Gas injector systems : For fabrication of nano structures. C deposition [Naphthalene: C10H6] Pt deposition [Methyl Cyclopentadienyl trimethyl Platinum: (CH3)3Pt(CpCH3)] W deposition [Tungsten Hexacarbonyl: W(CO)6] Insulator enhanced etch [Xenon Fluoride: XeF2] Enhanced etch [Iodine: I2] Residual gas analyzer (SRS RGA-300) : For analyzing the gases released during fabrication. Fast electron beam blanker (For electron beam lithography) Everhart-Thornley secondary electron detector Ultra thin Window sapphire detector (For EDS analysis) Usage and Applications: The Electron Beam is mainly utilized for insitu SEM imaging. The electron Beam can also be used for milling. The Electron Beam can also be utilized for electron beam lithography (EBL). In the Focused Ion Beam (FIB) system Ga+ ions are created, focused and accelerated toward a surface with large electric fields. The Ga+ ion beam can then be used to image or to nano-machine a surface. With the FIB we can build complex structures at the nanoscale. Most modern FIBs are combined with SEMs for easier operation and synergistic analysis. Ga+ is the most common LMIS used for commercial FIBs because it offers the best of all properties needed. Contacting of small structures by metal deposition. Non perpendicular sections. EDX line scan of mapping on a section. EBSD mapping on a section. Automated repeated cross sectioning 3D image TEM Lamella preparation. Deposition /milling with feature mill. Industrial Process Solution.

2 Carbon Cantilever for femto gram weight measurements A die in Silicon for fabrication of micron/nano size gear of polymers 50nm holes in NbSe2 for magnetic vortex characteristics Fabrication of Micro Squid with Nb thin Films Nano Electrodes

3 FIB System Components: A Vacuum system and chamber A liquid metal ion source An Ion column for milling and deposition Ion column consists of : Ga+ source (LMIS) ion optics (electrostatic lenses) fast beam blanker (electrostatic) different currents (aperture stripe) adjustable acceleration voltage An Electron column for imaging (SEM) A precision goniometer for sample mounting and manipulation Imaging detectors A gas injection system to spray a precursor gas on the sample surface Scan generators for ions and electrons Computer control.

4 Liquid Metal Ion Source(LMIS) LMIS Consists of a capillary tube with a needle through it an extraction electrode and a shielding. Capillary acts as a reservoir that feeds the metal to the tip. Heated Ga flows and wets the W needle having tip radius 2-5 µm. A suppresser voltage [electric field (10 8 V/cm)] applied to the end of the wetted tip causes the liquid Ga to form a point source (2-5 nm tip) in the shape of Taylor cone. Conical shapes forms because of electrostatic and surface tension force balance. An extraction voltage pulls Ga from the tip and efficiently ionize it by field evaporation of the metal at the end of the Taylor cone. Why Ga LMIS? 1. Low melting point (Tmp= C) minimizes any reaction of interdiffusion between the liquid and the W needle substrate. 2. Low volatility at the melting point conserves the supply of metal and yields a long source life. 3. Low surface energy promotes viscous behavior on the (usually W) substrate. 4. Low vapor pressure allows Ga to be used in its pure form instead of in the form of an alloy source and yields a long lifetime since the liquid will not evaporate. 5. Excellent mechanical, electrical, and vacuum properties. 6. Emission characteristics enable high angular intensity with a small energy spread. SEM imaging FIB imaging:(low ion current) Impinging Ga+ produce secondary electrons ET or in Lens detector Typically at 30 kv, 40 pa optimal resolution and signal Other currents and energies different contrast Advantages: Channeling contrast Removal of oxide layer Disadvantages: Damage of surface Remark : Now a days there is scanning He microscopy having high contrast and very high resolution

5 Focused Ion Beam (FIB): interaction with sample Ga+ beam hits the sample substrate and yields 1. Secondary electrons 2. Sputtered atoms and ions 3. Implantation of Ga 4. Amorphisation/recrystallization 5. Imaging, milling and deposition happen simultaneously Remarks: 1. Implantation and amorphisation also occur at grazing incidence. 2. Depth of damage layer depends also on energy of Ga+. Focused Ion Beam (FIB): Nano Scale milling (High ion current) For milling applications it is desirable that the incoming ions interact only with the atoms at the surface. If the ion energy (momentum) is adequate the collision can transfer sufficient energy to the surface atom to overcome its surface binding energy ( 3.8eV for Au and 4.7 ev for Si). Interaction solely depends on momentum transfer to remove the atoms, sputtering is purely a physical process. Note: There are other variants of the process like Reactive Ion Etching (RIE) where chemical species are incorporated and the process proceeds chemically Focused Ion Beam (FIB): deposition (Gas assisted) Focused ion beam scanning is our hand which defines the deposition area. Three dimensional nanostructures can be fabricated using layer by layer deposition. For FIB induced deposition, the necessary processes are Adsorption of the chemical precursor onto the sample surface. Decomposition of gas molecules into volatile and non volatile products by focused ion beam. Precursor must have two properties, namely : Sufficient sticking probability to stick to a surface of interest in sufficient quantity. Decompose more rapidly than it is sputtered away by the ion beam. Examples of species that can be deposited: C, Pt, W, Pd, SiO2

Focused Ion Beam Nanofabrication

Focused Ion Beam Nanofabrication Focused Ion Beam / Focused Electron Beam NT II - 2007 Focused Ion Beam Nanofabrication Nanotechnology for Engineers : J. Brugger (LMIS-1) & P. Hoffmann (IOA) Nova 600 NANOLAB (FEI) Dual-Beam Instrument

More information

Dual Beam Helios Nanolab 600 and 650

Dual Beam Helios Nanolab 600 and 650 Dual Beam Helios Nanolab 600 and 650 In the Clean Room facilities of the INA LMA, several lithography facilities permit to pattern structures at the micro and nano meter scale and to create devices. In

More information

Gaetano L Episcopo. Scanning Electron Microscopy Focus Ion Beam and. Pulsed Plasma Deposition

Gaetano L Episcopo. Scanning Electron Microscopy Focus Ion Beam and. Pulsed Plasma Deposition Gaetano L Episcopo Scanning Electron Microscopy Focus Ion Beam and Pulsed Plasma Deposition Hystorical background Scientific discoveries 1897: J. Thomson discovers the electron. 1924: L. de Broglie propose

More information

Outlines 3/12/2011. Vacuum Chamber. Inside the sample chamber. Nano-manipulator. Focused ion beam instrument. 1. Other components of FIB instrument

Outlines 3/12/2011. Vacuum Chamber. Inside the sample chamber. Nano-manipulator. Focused ion beam instrument. 1. Other components of FIB instrument Focused ion beam instruments Outlines 1. Other components of FIB instrument 1.a Vacuum chamber 1.b Nanomanipulator 1.c Gas supply for deposition 1.d Detectors 2. Capabilities of FIB instrument Lee Chow

More information

Electron beam scanning

Electron beam scanning Electron beam scanning The Electron beam scanning operates through an electro-optical system which has the task of deflecting the beam Synchronously with cathode ray tube which create the image, beam moves

More information

Table of Content. Mechanical Removing Techniques. Ultrasonic Machining (USM) Sputtering and Focused Ion Beam Milling (FIB)

Table of Content. Mechanical Removing Techniques. Ultrasonic Machining (USM) Sputtering and Focused Ion Beam Milling (FIB) Table of Content Mechanical Removing Techniques Ultrasonic Machining (USM) Sputtering and Focused Ion Beam Milling (FIB) Ultrasonic Machining In ultrasonic machining (USM), also called ultrasonic grinding,

More information

The Liquid Metal Ion Source A Hot Ion Source. Jon Orloff Professor Emeritus, University of Maryland and FEI Company Hillsboro, Oregon

The Liquid Metal Ion Source A Hot Ion Source. Jon Orloff Professor Emeritus, University of Maryland and FEI Company Hillsboro, Oregon The Liquid Metal Ion Source A Hot Ion Source Jon Orloff Professor Emeritus, University of Maryland and FEI Company Hillsboro, Oregon U.S. Northwest Pacific Coast 2 Introduction The main purpose of this

More information

LECTURE 5 SUMMARY OF KEY IDEAS

LECTURE 5 SUMMARY OF KEY IDEAS LECTURE 5 SUMMARY OF KEY IDEAS Etching is a processing step following lithography: it transfers a circuit image from the photoresist to materials form which devices are made or to hard masking or sacrificial

More information

Auger Electron Spectroscopy Overview

Auger Electron Spectroscopy Overview Auger Electron Spectroscopy Overview Also known as: AES, Auger, SAM 1 Auger Electron Spectroscopy E KLL = E K - E L - E L AES Spectra of Cu EdN(E)/dE Auger Electron E N(E) x 5 E KLL Cu MNN Cu LMM E f E

More information

EE 527 MICROFABRICATION. Lecture 24 Tai-Chang Chen University of Washington

EE 527 MICROFABRICATION. Lecture 24 Tai-Chang Chen University of Washington EE 527 MICROFABRICATION Lecture 24 Tai-Chang Chen University of Washington EDP ETCHING OF SILICON - 1 Ethylene Diamine Pyrocatechol Anisotropy: (100):(111) ~ 35:1 EDP is very corrosive, very carcinogenic,

More information

ORION NanoFab: An Overview of Applications. White Paper

ORION NanoFab: An Overview of Applications. White Paper ORION NanoFab: An Overview of Applications White Paper ORION NanoFab: An Overview of Applications Author: Dr. Bipin Singh Carl Zeiss NTS, LLC, USA Date: September 2012 Introduction With the advancement

More information

TMT4320 Nanomaterials November 10 th, Thin films by physical/chemical methods (From chapter 24 and 25)

TMT4320 Nanomaterials November 10 th, Thin films by physical/chemical methods (From chapter 24 and 25) 1 TMT4320 Nanomaterials November 10 th, 2015 Thin films by physical/chemical methods (From chapter 24 and 25) 2 Thin films by physical/chemical methods Vapor-phase growth (compared to liquid-phase growth)

More information

MSN551 LITHOGRAPHY II

MSN551 LITHOGRAPHY II MSN551 Introduction to Micro and Nano Fabrication LITHOGRAPHY II E-Beam, Focused Ion Beam and Soft Lithography Why need electron beam lithography? Smaller features are required By electronics industry:

More information

Imaging Methods: Scanning Force Microscopy (SFM / AFM)

Imaging Methods: Scanning Force Microscopy (SFM / AFM) Imaging Methods: Scanning Force Microscopy (SFM / AFM) The atomic force microscope (AFM) probes the surface of a sample with a sharp tip, a couple of microns long and often less than 100 Å in diameter.

More information

ETCHING Chapter 10. Mask. Photoresist

ETCHING Chapter 10. Mask. Photoresist ETCHING Chapter 10 Mask Light Deposited Substrate Photoresist Etch mask deposition Photoresist application Exposure Development Etching Resist removal Etching of thin films and sometimes the silicon substrate

More information

Lecture 15: Introduction to mass spectrometry-i

Lecture 15: Introduction to mass spectrometry-i Lecture 15: Introduction to mass spectrometry-i Mass spectrometry (MS) is an analytical technique that measures the mass/charge ratio of charged particles in vacuum. Mass spectrometry can determine masse/charge

More information

CHAPTER 6: Etching. Chapter 6 1

CHAPTER 6: Etching. Chapter 6 1 Chapter 6 1 CHAPTER 6: Etching Different etching processes are selected depending upon the particular material to be removed. As shown in Figure 6.1, wet chemical processes result in isotropic etching

More information

Part II: Thin Film Characterization

Part II: Thin Film Characterization Part II: Thin Film Characterization General details of thin film characterization instruments 1. Introduction to Thin Film Characterization Techniques 2. Structural characterization: SEM, TEM, AFM, STM

More information

Basic structure of SEM

Basic structure of SEM Table of contents Basis structure of SEM SEM imaging modes Comparison of ordinary SEM and FESEM Electron behavior Electron matter interaction o Elastic interaction o Inelastic interaction o Interaction

More information

Supplementary Figure 1 Detailed illustration on the fabrication process of templatestripped

Supplementary Figure 1 Detailed illustration on the fabrication process of templatestripped Supplementary Figure 1 Detailed illustration on the fabrication process of templatestripped gold substrate. (a) Spin coating of hydrogen silsesquioxane (HSQ) resist onto the silicon substrate with a thickness

More information

SOLID STATE PHYSICS PHY F341. Dr. Manjuladevi.V Associate Professor Department of Physics BITS Pilani

SOLID STATE PHYSICS PHY F341. Dr. Manjuladevi.V Associate Professor Department of Physics BITS Pilani SOLID STATE PHYSICS PHY F341 Dr. Manjuladevi.V Associate Professor Department of Physics BITS Pilani 333031 manjula@bits-pilani.ac.in Characterization techniques SEM AFM STM BAM Outline What can we use

More information

Micromachining structured optical fibres using focused ion. beam (FIB) milling

Micromachining structured optical fibres using focused ion. beam (FIB) milling Micromachining structured optical fibres using focused ion beam (FIB) milling Cicero Martelli Optical Fibre Technology Centre, School of Chemistry, University of Sydney, 206 National Innovation Centre,

More information

Secondary ion mass spectrometry (SIMS)

Secondary ion mass spectrometry (SIMS) Secondary ion mass spectrometry (SIMS) ELEC-L3211 Postgraduate Course in Micro and Nanosciences Department of Micro and Nanosciences Personal motivation and experience on SIMS Offers the possibility to

More information

Introduction to Electron Beam Lithography

Introduction to Electron Beam Lithography Introduction to Electron Beam Lithography Boštjan Berčič (bostjan.bercic@ijs.si), Jožef Štefan Institute, Jamova 39, 1000 Ljubljana, Slovenia 1. Introduction Electron Beam Lithography is a specialized

More information

Vapor-Phase Cutting of Carbon Nanotubes Using a Nanomanipulator Platform

Vapor-Phase Cutting of Carbon Nanotubes Using a Nanomanipulator Platform Vapor-Phase Cutting of Carbon Nanotubes Using a Nanomanipulator Platform MS&T 10, October 18, 2010 Vladimir Mancevski, President and CTO, Xidex Corporation Philip D. Rack, Professor, The University of

More information

PHI 5000 Versaprobe-II Focus X-ray Photo-electron Spectroscopy

PHI 5000 Versaprobe-II Focus X-ray Photo-electron Spectroscopy PHI 5000 Versaprobe-II Focus X-ray Photo-electron Spectroscopy The very basic theory of XPS XPS theroy Surface Analysis Ultra High Vacuum (UHV) XPS Theory XPS = X-ray Photo-electron Spectroscopy X-ray

More information

Nanostructure. Materials Growth Characterization Fabrication. More see Waser, chapter 2

Nanostructure. Materials Growth Characterization Fabrication. More see Waser, chapter 2 Nanostructure Materials Growth Characterization Fabrication More see Waser, chapter 2 Materials growth - deposition deposition gas solid Physical Vapor Deposition Chemical Vapor Deposition Physical Vapor

More information

Chapter 6. Superconducting Quantum Circuits

Chapter 6. Superconducting Quantum Circuits AS-Chap. 6.1-1 Chapter 6 Superconducting Quantum Circuits AS-Chap. 6.1-2 6.1 Fabrication of JJ for quantum circuits AS-Chap. 6.1-3 Motivation Repetition Current-phase and voltage-phase relation are classical,

More information

ICPMS Doherty Lecture 1

ICPMS Doherty Lecture 1 ICPMS Doherty Lecture 1 Mass Spectrometry This material provides some background on how to measure isotope abundances by means of mass spectrometry. Mass spectrometers create and separate ionized atoms

More information

Chemistry Instrumental Analysis Lecture 34. Chem 4631

Chemistry Instrumental Analysis Lecture 34. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 34 From molecular to elemental analysis there are three major techniques used for elemental analysis: Optical spectrometry Mass spectrometry X-ray spectrometry

More information

Metal Deposition. Filament Evaporation E-beam Evaporation Sputter Deposition

Metal Deposition. Filament Evaporation E-beam Evaporation Sputter Deposition Metal Deposition Filament Evaporation E-beam Evaporation Sputter Deposition 1 Filament evaporation metals are raised to their melting point by resistive heating under vacuum metal pellets are placed on

More information

Device Characterization of 0.21 µm CMOS Device

Device Characterization of 0.21 µm CMOS Device Device Characterization of 0.21 µm CMOS Device Lim Teck Foo 1 *, Ibrahim Ahmad 2 and Muhammad Suhaimi Sulong 3 1 Department of Product Engineering, Altera Corporation. 2 Department of Electrical, Electronics,

More information

Etching Issues - Anisotropy. Dry Etching. Dry Etching Overview. Etching Issues - Selectivity

Etching Issues - Anisotropy. Dry Etching. Dry Etching Overview. Etching Issues - Selectivity Etching Issues - Anisotropy Dry Etching Dr. Bruce K. Gale Fundamentals of Micromachining BIOEN 6421 EL EN 5221 and 6221 ME EN 5960 and 6960 Isotropic etchants etch at the same rate in every direction mask

More information

Nanostructures Fabrication Methods

Nanostructures Fabrication Methods Nanostructures Fabrication Methods bottom-up methods ( atom by atom ) In the bottom-up approach, atoms, molecules and even nanoparticles themselves can be used as the building blocks for the creation of

More information

Everhart-Thornley detector

Everhart-Thornley detector SEI Detector Everhart-Thornley detector Microscope chamber wall Faraday cage Scintillator Electrons in Light pipe Photomultiplier Electrical signal out Screen Quartz window +200 V +10 kv Always contains

More information

= 6 (1/ nm) So what is probability of finding electron tunneled into a barrier 3 ev high?

= 6 (1/ nm) So what is probability of finding electron tunneled into a barrier 3 ev high? STM STM With a scanning tunneling microscope, images of surfaces with atomic resolution can be readily obtained. An STM uses quantum tunneling of electrons to map the density of electrons on the surface

More information

CBE Science of Engineering Materials. Scanning Electron Microscopy (SEM)

CBE Science of Engineering Materials. Scanning Electron Microscopy (SEM) CBE 30361 Science of Engineering Materials Scanning Electron Microscopy (SEM) Scale of Structure Organization Units: micrometer = 10-6 m = 1µm nanometer= 10-9 m = 1nm Angstrom = 10-10 m = 1Å A hair is

More information

The illumination source: the electron beam

The illumination source: the electron beam The SEM Column The illumination source: the electron beam The probe of the electron microscope is an electron beam with very high and stable energy (10-100 kev) in order to get images with high resolution.

More information

Fadei Komarov Alexander Kamyshan

Fadei Komarov Alexander Kamyshan Fadei Komarov Alexander Kamyshan Institute of Applied Physics Problems, Belarusian State University, Minsk, Belarus KomarovF@bsu.by Tasks and Objects 2 Introduction and motivation Experimental setup designed

More information

6.5 Optical-Coating-Deposition Technologies

6.5 Optical-Coating-Deposition Technologies 92 Chapter 6 6.5 Optical-Coating-Deposition Technologies The coating process takes place in an evaporation chamber with a fully controlled system for the specified requirements. Typical systems are depicted

More information

High Yield Structured X-ray Photo-Cathode Development and Fabrication

High Yield Structured X-ray Photo-Cathode Development and Fabrication High Yield Structured X-ray Photo-Cathode Development and Fabrication K. Opachich 1, P. Ross 1, J. Koch 1, A. MacPhee 2, O. Landen 2, D. Bradley 2, P. Bell 2, S. Nagel 2, T. Hilsabeck 4, N. Chen 5, S.

More information

Chapter 9. Electron mean free path Microscopy principles of SEM, TEM, LEEM

Chapter 9. Electron mean free path Microscopy principles of SEM, TEM, LEEM Chapter 9 Electron mean free path Microscopy principles of SEM, TEM, LEEM 9.1 Electron Mean Free Path 9. Scanning Electron Microscopy (SEM) -SEM design; Secondary electron imaging; Backscattered electron

More information

Fabrication at the nanoscale for nanophotonics

Fabrication at the nanoscale for nanophotonics Fabrication at the nanoscale for nanophotonics Ilya Sychugov, KTH Materials Physics, Kista silicon nanocrystal by electron beam induced deposition lithography Outline of basic nanofabrication methods Devices

More information

3.155J/6.152J Microelectronic Processing Technology Fall Term, 2004

3.155J/6.152J Microelectronic Processing Technology Fall Term, 2004 3.155J/6.152J Microelectronic Processing Technology Fall Term, 2004 Bob O'Handley Martin Schmidt Quiz Nov. 17, 2004 Ion implantation, diffusion [15] 1. a) Two identical p-type Si wafers (N a = 10 17 cm

More information

Ecole Franco-Roumaine : Magnétisme des systèmes nanoscopiques et structures hybrides - Brasov, Modern Analytical Microscopic Tools

Ecole Franco-Roumaine : Magnétisme des systèmes nanoscopiques et structures hybrides - Brasov, Modern Analytical Microscopic Tools 1. Introduction Solid Surfaces Analysis Group, Institute of Physics, Chemnitz University of Technology, Germany 2. Limitations of Conventional Optical Microscopy 3. Electron Microscopies Transmission Electron

More information

Ionic Liquid Ion Sources in the Processing of Materials and Other Applications

Ionic Liquid Ion Sources in the Processing of Materials and Other Applications Ionic Liquid Ion Sources in the Processing of Materials and Other Applications Paulo Lozano Massachusetts Institute of Technology Materials and Processes Far From Equilibrium Workshop November 3, 2010

More information

Final exam: take-home part

Final exam: take-home part Final exam: take-home part! List five things that can be done to improve this class. Be specific; give much detail.! (You will be penalized only for insulting comments made for no benefit; you will not

More information

TESCAN S New generation of FIB-SEM microscope

TESCAN S New generation of FIB-SEM microscope TESCAN S New generation of FIB-SEM microscope rising standards in sample preparation Key Features SEM COLUMN Versatile system for unlimited applications: resolution imaging (0.9 nm at 15 kev, 1.4 nm at

More information

An environment designed for success

An environment designed for success An environment designed for success The nanofab is a centralized, open-access, training, service, and collaboration facility, focused on academic research and industrial applications in micro- and nanoscale

More information

Introduction to X-ray Photoelectron Spectroscopy (XPS) XPS which makes use of the photoelectric effect, was developed in the mid-1960

Introduction to X-ray Photoelectron Spectroscopy (XPS) XPS which makes use of the photoelectric effect, was developed in the mid-1960 Introduction to X-ray Photoelectron Spectroscopy (XPS) X-ray Photoelectron Spectroscopy (XPS), also known as Electron Spectroscopy for Chemical Analysis (ESCA) is a widely used technique to investigate

More information

Repetition: Ion Plating

Repetition: Ion Plating Repetition: Ion Plating Substrate HV (bis ca. 1kV) Optional ionization system Source Ionized filling gas Source material, ionized or neutral Repetition: Ion Plating Ion Species Separated ion source Ions

More information

Lecture 6 Plasmas. Chapters 10 &16 Wolf and Tauber. ECE611 / CHE611 Electronic Materials Processing Fall John Labram 1/68

Lecture 6 Plasmas. Chapters 10 &16 Wolf and Tauber. ECE611 / CHE611 Electronic Materials Processing Fall John Labram 1/68 Lecture 6 Plasmas Chapters 10 &16 Wolf and Tauber 1/68 Announcements Homework: Homework will be returned to you on Thursday (12 th October). Solutions will be also posted online on Thursday (12 th October)

More information

How to distinguish EUV photons from out-of-band photons

How to distinguish EUV photons from out-of-band photons How to distinguish EUV photons from out-of-band photons Thesis submitted in partial fulfillment of the requirements for the degree of Master of Science in Physics Author: Student ID: Supervisors: 2 nd

More information

MS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS

MS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS 2016 Fall Semester MS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS Byungha Shin Dept. of MSE, KAIST 1 Course Information Syllabus 1. Overview of various characterization techniques (1 lecture)

More information

Kavli Workshop for Journalists. June 13th, CNF Cleanroom Activities

Kavli Workshop for Journalists. June 13th, CNF Cleanroom Activities Kavli Workshop for Journalists June 13th, 2007 CNF Cleanroom Activities Seeing nm-sized Objects with an SEM Lab experience: Scanning Electron Microscopy Equipment: Zeiss Supra 55VP Scanning electron microscopes

More information

Scanning Electron Microscopy

Scanning Electron Microscopy Scanning Electron Microscopy Field emitting tip Grid 2kV 100kV Anode ZEISS SUPRA Variable Pressure FESEM Dr Heath Bagshaw CMA bagshawh@tcd.ie Why use an SEM? Fig 1. Examples of features resolvable using

More information

High Yield Structured X-ray Photo-Cathode Development and Fabrication

High Yield Structured X-ray Photo-Cathode Development and Fabrication High Yield Structured X-ray Photo-Cathode Development and Fabrication K. Opachich, P. Ross, J. Koch (NSTec, LLC) A. MacPhee, O. Landen, D. Bradley, P. Bell, S. Nagel (LLNL) T. Hilsabeck (GA) N. Chen, S.

More information

object objective lens eyepiece lens

object objective lens eyepiece lens Advancing Physics G495 June 2015 SET #1 ANSWERS Field and Particle Pictures Seeing with electrons The compound optical microscope Q1. Before attempting this question it may be helpful to review ray diagram

More information

Chapter 10. Nanometrology. Oxford University Press All rights reserved.

Chapter 10. Nanometrology. Oxford University Press All rights reserved. Chapter 10 Nanometrology Oxford University Press 2013. All rights reserved. 1 Introduction Nanometrology is the science of measurement at the nanoscale level. Figure illustrates where nanoscale stands

More information

MSE 321 Structural Characterization

MSE 321 Structural Characterization Optical Microscope Plan Lenses In an "ideal" single-element lens system all planar wave fronts are focused to a point at distance f from the lens; therefore: Image near the optical axis will be in perfect

More information

Scanning Electron Microscopy

Scanning Electron Microscopy Scanning Electron Microscopy Amanpreet Kaur 1 www.reading.ac.uk/emlab Scanning Electron Microscopy What is scanning electron microscopy? Basic features of conventional SEM Limitations of conventional SEM

More information

Secondary Ion Mass Spectroscopy (SIMS)

Secondary Ion Mass Spectroscopy (SIMS) Secondary Ion Mass Spectroscopy (SIMS) Analyzing Inorganic Solids * = under special conditions ** = semiconductors only + = limited number of elements or groups Analyzing Organic Solids * = under special

More information

Chapter 10. Superconducting Quantum Circuits

Chapter 10. Superconducting Quantum Circuits AS-Chap. 10-1 Chapter 10 Superconducting Quantum Circuits AS-Chap. 10-2 10.1 Fabrication of JJ for quantum circuits AS-Chap. 10-3 Motivation Repetition Current-phase and voltage-phase relation are classical,

More information

Wet and Dry Etching. Theory

Wet and Dry Etching. Theory Wet and Dry Etching Theory 1. Introduction Etching techniques are commonly used in the fabrication processes of semiconductor devices to remove selected layers for the purposes of pattern transfer, wafer

More information

There's Plenty of Room at the Bottom

There's Plenty of Room at the Bottom There's Plenty of Room at the Bottom 12/29/1959 Feynman asked why not put the entire Encyclopedia Britannica (24 volumes) on a pin head (requires atomic scale recording). He proposed to use electron microscope

More information

Technology for Micro- and Nanostructures Micro- and Nanotechnology

Technology for Micro- and Nanostructures Micro- and Nanotechnology Lecture 5: Electron-Beam Lithography, Part 1 Technology for Micro- and Nanostructures Micro- and Nanotechnology Peter Unger mailto: peter.unger @ uni-ulm.de Institute of Optoelectronics University of Ulm

More information

Secondary Ion Mass Spectrometry (SIMS) Thomas Sky

Secondary Ion Mass Spectrometry (SIMS) Thomas Sky 1 Secondary Ion Mass Spectrometry (SIMS) Thomas Sky Depth (µm) 2 Characterization of solar cells 0,0 1E16 1E17 1E18 1E19 1E20 0,2 0,4 0,6 0,8 1,0 1,2 P Concentration (cm -3 ) Characterization Optimization

More information

Mass Spectrometry in MCAL

Mass Spectrometry in MCAL Mass Spectrometry in MCAL Two systems: GC-MS, LC-MS GC seperates small, volatile, non-polar material MS is detection devise (Agilent 320-MS TQ Mass Spectrometer) Full scan monitoring SIM single ion monitoring

More information

Single ion implantation for nanoelectronics and the application to biological systems. Iwao Ohdomari Waseda University Tokyo, Japan

Single ion implantation for nanoelectronics and the application to biological systems. Iwao Ohdomari Waseda University Tokyo, Japan Single ion implantation for nanoelectronics and the application to biological systems Iwao Ohdomari Waseda University Tokyo, Japan Contents 1.History of single ion implantation (SII) 2.Novel applications

More information

Plasma etching. Bibliography

Plasma etching. Bibliography Plasma etching Bibliography 1. B. Chapman, Glow discharge processes, (Wiley, New York, 1980). - Classical plasma processing of etching and sputtering 2. D. M. Manos and D. L. Flamm, Plasma etching; An

More information

Direct-Write Deposition Utilizing a Focused Electron Beam

Direct-Write Deposition Utilizing a Focused Electron Beam Direct-Write Deposition Utilizing a Focused Electron Beam M. Fischer, J. Gottsbachner, S. Müller, W. Brezna, and H.D. Wanzenboeck Institute of Solid State Electronics, Vienna University of Technology,

More information

AP5301/ Name the major parts of an optical microscope and state their functions.

AP5301/ Name the major parts of an optical microscope and state their functions. Review Problems on Optical Microscopy AP5301/8301-2015 1. Name the major parts of an optical microscope and state their functions. 2. Compare the focal lengths of two glass converging lenses, one with

More information

Repetition: Practical Aspects

Repetition: Practical Aspects Repetition: Practical Aspects Reduction of the Cathode Dark Space! E x 0 Geometric limit of the extension of a sputter plant. Lowest distance between target and substrate V Cathode (Target/Source) - +

More information

Auger Electron Spectroscopy

Auger Electron Spectroscopy Auger Electron Spectroscopy Auger Electron Spectroscopy is an analytical technique that provides compositional information on the top few monolayers of material. Detect all elements above He Detection

More information

Electron Microprobe Analysis 1 Nilanjan Chatterjee, Ph.D. Principal Research Scientist

Electron Microprobe Analysis 1 Nilanjan Chatterjee, Ph.D. Principal Research Scientist 12.141 Electron Microprobe Analysis 1 Nilanjan Chatterjee, Ph.D. Principal Research Scientist Massachusetts Institute of Technology Electron Microprobe Facility Department of Earth, Atmospheric and Planetary

More information

Electron Microprobe Analysis 1 Nilanjan Chatterjee, Ph.D. Principal Research Scientist

Electron Microprobe Analysis 1 Nilanjan Chatterjee, Ph.D. Principal Research Scientist 12.141 Electron Microprobe Analysis 1 Nilanjan Chatterjee, Ph.D. Principal Research Scientist Massachusetts Institute of Technology Electron Microprobe Facility Department of Earth, Atmospheric and Planetary

More information

High-density data storage: principle

High-density data storage: principle High-density data storage: principle Current approach High density 1 bit = many domains Information storage driven by domain wall shifts 1 bit = 1 magnetic nanoobject Single-domain needed Single easy axis

More information

Precision Cutting and Patterning of Graphene with Helium Ions. 1.School of Engineering and Applied Sciences, Harvard University, Cambridge MA 02138

Precision Cutting and Patterning of Graphene with Helium Ions. 1.School of Engineering and Applied Sciences, Harvard University, Cambridge MA 02138 Precision Cutting and Patterning of Graphene with Helium Ions D.C. Bell 1,2, M.C. Lemme 3, L. A. Stern 4, J.R. Williams 1,3, C. M. Marcus 3 1.School of Engineering and Applied Sciences, Harvard University,

More information

Low Vacuum Scanning Electron Microscopy and Microanalysis

Low Vacuum Scanning Electron Microscopy and Microanalysis Low Vacuum Scanning Electron Microscopy and Microanalysis Principles and Practice of Variable Pressure/Environmental Scanning Electron Microscopy (VP-ESEM), Debbie J Stokes, John Wiley&Sons 2008 Several

More information

High brightness inductively coupled plasma source for high current focused ion beam applications

High brightness inductively coupled plasma source for high current focused ion beam applications High brightness inductively coupled plasma source for high current focused ion beam applications N. S. Smith, a W. P. Skoczylas, S. M. Kellogg, D. E. Kinion, and P. P. Tesch FEI Company, 5350 NE Dawson

More information

Two-Dimensional (C 4 H 9 NH 3 ) 2 PbBr 4 Perovskite Crystals for. High-Performance Photodetector. Supporting Information for

Two-Dimensional (C 4 H 9 NH 3 ) 2 PbBr 4 Perovskite Crystals for. High-Performance Photodetector. Supporting Information for Supporting Information for Two-Dimensional (C 4 H 9 NH 3 ) 2 PbBr 4 Perovskite Crystals for High-Performance Photodetector Zhenjun Tan,,ǁ, Yue Wu,ǁ, Hao Hong, Jianbo Yin, Jincan Zhang,, Li Lin, Mingzhan

More information

Keywords- Focused Ion Beams, Nanostructuring, Polymers, Functionalization, Electron Microscopy, Surface Modification

Keywords- Focused Ion Beams, Nanostructuring, Polymers, Functionalization, Electron Microscopy, Surface Modification THE USE OF FOCUSED ELECTRON AND ION BEAMS FOR THE FUNCTIONALIZATION AND NANOSTRUCTURING OF POLYMER SURFACES 1 MELTEM SEZEN, 2 FERAY BAKAN 1,2 SUNUM Sabanci University Turkey E-mail: 1 meltemsezen@sabanciuniv.edu,

More information

SUPPLEMENTARY MATERIALS FOR PHONON TRANSMISSION COEFFICIENTS AT SOLID INTERFACES

SUPPLEMENTARY MATERIALS FOR PHONON TRANSMISSION COEFFICIENTS AT SOLID INTERFACES 148 A p p e n d i x D SUPPLEMENTARY MATERIALS FOR PHONON TRANSMISSION COEFFICIENTS AT SOLID INTERFACES D.1 Overview The supplementary information contains additional information on our computational approach

More information

HOW TO APPROACH SCANNING ELECTRON MICROSCOPY AND ENERGY DISPERSIVE SPECTROSCOPY ANALYSIS. SCSAM Short Course Amir Avishai

HOW TO APPROACH SCANNING ELECTRON MICROSCOPY AND ENERGY DISPERSIVE SPECTROSCOPY ANALYSIS. SCSAM Short Course Amir Avishai HOW TO APPROACH SCANNING ELECTRON MICROSCOPY AND ENERGY DISPERSIVE SPECTROSCOPY ANALYSIS SCSAM Short Course Amir Avishai RESEARCH QUESTIONS Sea Shell Cast Iron EDS+SE Fe Cr C Objective Ability to ask the

More information

FIB Etching and Deposition on Nanoscale Studied by TEM and Numerical Modeling

FIB Etching and Deposition on Nanoscale Studied by TEM and Numerical Modeling FIB Etching and Deposition on Nanoscale Studied by TEM and Numerical Modeling V. Ray, E. Chang, Sz.C. Liou, K. Toula, and W.A. Chiou vray@umd.edu 8 th FIB/SEM Workshop, John Hopkins APL, Laurel MD Outline

More information

Effect of Spiral Microwave Antenna Configuration on the Production of Nano-crystalline Film by Chemical Sputtering in ECR Plasma

Effect of Spiral Microwave Antenna Configuration on the Production of Nano-crystalline Film by Chemical Sputtering in ECR Plasma THE HARRIS SCIENCE REVIEW OF DOSHISHA UNIVERSITY, VOL. 56, No. 1 April 2015 Effect of Spiral Microwave Antenna Configuration on the Production of Nano-crystalline Film by Chemical Sputtering in ECR Plasma

More information

UNIT 3. By: Ajay Kumar Gautam Asst. Prof. Dev Bhoomi Institute of Technology & Engineering, Dehradun

UNIT 3. By: Ajay Kumar Gautam Asst. Prof. Dev Bhoomi Institute of Technology & Engineering, Dehradun UNIT 3 By: Ajay Kumar Gautam Asst. Prof. Dev Bhoomi Institute of Technology & Engineering, Dehradun 1 Syllabus Lithography: photolithography and pattern transfer, Optical and non optical lithography, electron,

More information

M2 TP. Low-Energy Electron Diffraction (LEED)

M2 TP. Low-Energy Electron Diffraction (LEED) M2 TP Low-Energy Electron Diffraction (LEED) Guide for report preparation I. Introduction: Elastic scattering or diffraction of electrons is the standard technique in surface science for obtaining structural

More information

Ion beam lithography

Ion beam lithography Ion beam lithography Progress in ion technology spot size

More information

MSE 321 Structural Characterization

MSE 321 Structural Characterization Auger Spectroscopy Auger Electron Spectroscopy (AES) Scanning Auger Microscopy (SAM) Incident Electron Ejected Electron Auger Electron Initial State Intermediate State Final State Physical Electronics

More information

MICROCHIP MANUFACTURING by S. Wolf

MICROCHIP MANUFACTURING by S. Wolf by S. Wolf Chapter 15 ALUMINUM THIN-FILMS and SPUTTER-DEPOSITION 2004 by LATTICE PRESS CHAPTER 15 - CONTENTS Aluminum Thin-Films Sputter-Deposition Process Steps Physics of Sputter-Deposition Magnetron-Sputtering

More information

Nanoholes for leak metrology

Nanoholes for leak metrology Vacuum Metrology for Industry Nanoholes for leak metrology Università Degli Studi di Genova, Italy OUTLINE INTRODUCTION FABRICATION OF NANOHOLES GEOMETRICAL CHARACTERIZATION LEAK DEVICES RESULTS: PTB INRIM

More information

X-Ray Photoelectron Spectroscopy (XPS) Prof. Paul K. Chu

X-Ray Photoelectron Spectroscopy (XPS) Prof. Paul K. Chu X-Ray Photoelectron Spectroscopy (XPS) Prof. Paul K. Chu X-ray Photoelectron Spectroscopy Introduction Qualitative analysis Quantitative analysis Charging compensation Small area analysis and XPS imaging

More information

MSE 321 Structural Characterization

MSE 321 Structural Characterization Auger Spectroscopy Auger Electron Spectroscopy (AES) Scanning Auger Microscopy (SAM) Incident Electron Ejected Electron Auger Electron Initial State Intermediate State Final State Physical Electronics

More information

Slow-Positron-Beam Techniques

Slow-Positron-Beam Techniques Slow-Positron-Beam Techniques 1 Slow-Positron-Beam Techniques The main advantage of the conventional sample source sandwich arrangement is that the emitted positrons immediately penetrate the sample. A

More information

Focused-ion-beam milling based nanostencil mask fabrication for spin transfer torque studies. Güntherodt

Focused-ion-beam milling based nanostencil mask fabrication for spin transfer torque studies. Güntherodt Focused-ion-beam milling based nanostencil mask fabrication for spin transfer torque studies B. Özyilmaz a, G. Richter, N. Müsgens, M. Fraune, M. Hawraneck, B. Beschoten b, and G. Güntherodt Physikalisches

More information

Low Voltage Field Emission SEM (LV FE-SEM): A Promising Imaging Approach for Graphene Samples

Low Voltage Field Emission SEM (LV FE-SEM): A Promising Imaging Approach for Graphene Samples Low Voltage Field Emission SEM (LV FE-SEM): A Promising Imaging Approach for Graphene Samples Jining Xie Agilent Technologies May 23 rd, 2012 www.agilent.com/find/nano Outline 1. Introduction 2. Agilent

More information

h p λ = mν Back to de Broglie and the electron as a wave you will learn more about this Equation in CHEM* 2060

h p λ = mν Back to de Broglie and the electron as a wave you will learn more about this Equation in CHEM* 2060 Back to de Broglie and the electron as a wave λ = mν h = h p you will learn more about this Equation in CHEM* 2060 We will soon see that the energies (speed for now if you like) of the electrons in the

More information

Atomic Force/Magnetic Force Microscope

Atomic Force/Magnetic Force Microscope Atomic Force/Magnetic Force Microscope Veeco Instruments Dimension 3000 SPM with Nanoscope IIIa controller Atomic Force Microscopy Mode Magnetic Force Microscopy Mode Vibration isolation and sound proof

More information

Secondaryionmassspectrometry

Secondaryionmassspectrometry Secondaryionmassspectrometry (SIMS) 1 Incident Ion Techniques for Surface Composition Analysis Mass spectrometric technique 1. Ionization -Electron ionization (EI) -Chemical ionization (CI) -Field ionization

More information