Nova 600 NanoLab Dual beam Focused Ion Beam IITKanpur

Similar documents
Focused Ion Beam Nanofabrication

Dual Beam Helios Nanolab 600 and 650

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

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

Electron beam scanning

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

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

LECTURE 5 SUMMARY OF KEY IDEAS

Auger Electron Spectroscopy Overview

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

ORION NanoFab: An Overview of Applications. White Paper

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

MSN551 LITHOGRAPHY II

Imaging Methods: Scanning Force Microscopy (SFM / AFM)

ETCHING Chapter 10. Mask. Photoresist

Lecture 15: Introduction to mass spectrometry-i

CHAPTER 6: Etching. Chapter 6 1

Part II: Thin Film Characterization

Basic structure of SEM

Supplementary Figure 1 Detailed illustration on the fabrication process of templatestripped

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

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

Secondary ion mass spectrometry (SIMS)

Introduction to Electron Beam Lithography

Vapor-Phase Cutting of Carbon Nanotubes Using a Nanomanipulator Platform

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

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

Chapter 6. Superconducting Quantum Circuits

ICPMS Doherty Lecture 1

Chemistry Instrumental Analysis Lecture 34. Chem 4631

Metal Deposition. Filament Evaporation E-beam Evaporation Sputter Deposition

Device Characterization of 0.21 µm CMOS Device

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

Nanostructures Fabrication Methods

Everhart-Thornley detector

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

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

The illumination source: the electron beam

Fadei Komarov Alexander Kamyshan

6.5 Optical-Coating-Deposition Technologies

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

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

Fabrication at the nanoscale for nanophotonics

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

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

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

Final exam: take-home part

TESCAN S New generation of FIB-SEM microscope

An environment designed for success

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

Repetition: Ion Plating

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

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

MS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS

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

Scanning Electron Microscopy

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

object objective lens eyepiece lens

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

MSE 321 Structural Characterization

Scanning Electron Microscopy

Secondary Ion Mass Spectroscopy (SIMS)

Chapter 10. Superconducting Quantum Circuits

Wet and Dry Etching. Theory

There's Plenty of Room at the Bottom

Technology for Micro- and Nanostructures Micro- and Nanotechnology

Secondary Ion Mass Spectrometry (SIMS) Thomas Sky

Mass Spectrometry in MCAL

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

Plasma etching. Bibliography

Direct-Write Deposition Utilizing a Focused Electron Beam

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

Repetition: Practical Aspects

Auger Electron Spectroscopy

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

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

High-density data storage: principle

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

Low Vacuum Scanning Electron Microscopy and Microanalysis

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

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

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

SUPPLEMENTARY MATERIALS FOR PHONON TRANSMISSION COEFFICIENTS AT SOLID INTERFACES

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

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

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

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

M2 TP. Low-Energy Electron Diffraction (LEED)

Ion beam lithography

MSE 321 Structural Characterization

MICROCHIP MANUFACTURING by S. Wolf

Nanoholes for leak metrology

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

MSE 321 Structural Characterization

Slow-Positron-Beam Techniques

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

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

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

Atomic Force/Magnetic Force Microscope

Secondaryionmassspectrometry

Transcription:

Nova 600 NanoLab Dual beam Focused Ion Beam system @ 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 600000X 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.

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

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.

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= 29.8 0 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

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