Hong Koh Yiin -CAMTEC 2011- 1 Image from:

Slides:



Advertisements
Similar presentations
Ge 116 Module 1: Scanning Electron Microscopy
Advertisements

General Characteristics of Gas Detectors
Production of X-rays (1)
Focused ion beam (FIB) 1.Overview. 2.Ion source and optics. 3.Ion-solid interaction, damage. 4.Scanning ion beam imaging. ECE 730: Fabrication in the nanoscale:
SEM & TEM in Polymer Characterization
Electron-Specimen Interactions
Scanning Electron Microscope (SEM)
Groups: WA 2,4,5,7. History  The electron microscope was first invented by a team of German engineers headed by Max Knoll and physicist Ernst Ruska in.
Effect of Accelerating Voltage on Resolution
Introduction Secondary electron secondary electron detector The electron beam interaction with near surface specimen atoms will make a signal which results.
Prime Exposure Factors II By Professor Stelmark. Primary Factors The primary exposure technique factors the radiographer selects on the control panel.
X-radiation. X-rays are part of the electromagnetic spectrum. X-radiation (composed of X-rays) is a form of electromagnetic radiation. X- rays have a.
Electron-Specimen Interactions
Lecture 5.1 Scanning Electron Microscopy (SEM)
Types of Radiation Interactions All or Nothing Many Small There is a finite probability per unit length that the radiation is absorbed. If not, there is.
XPS and SIMS MSN 506 Notes.
Scanning Electron Microscope Jamie Goings. Theory Conventional microscopes use light and glass lenses SEM uses electrons and magnetic lenses to create.
Instrumental Chemistry Chapter 12 Atomic X-Ray Spectroscopic.
Scanning Electron Microscope د. عمر عبد القادر.
Surface Emissions Specimen current X-rays Cathodoluminescence Pole Piece, etc SE3  ≈ 1 nm for metals up to 10 nm for insulators.
SEM microscope By: Doug, Holly & Oleg. Scanning Electron Microscope vs. Optical Microscope Advantages Continuously variable magnification High resolution.
BY SANTANU PRAMANIK(09369) HITESH KUMAR GUPTA(09320) CHANDAN SINGH(09260) SCANNING ELECTRON MICROSCOPE MATERIAL SCIENCE ASSIGNMENT.
8.1 PRODUCTION AND CHARACTERISTICS OF X-RAYS
Do it with electrons !. Microscopy Structure determines properties We have discussed crystal structure (x-ray diffraction) But consider now different.
Elsevier items and derived items © 2009 by Mosby, Inc., an affiliate of Elsevier Inc. X-Ray Production Chapter 8.
1 M. Aslam Baig National Center for Physics Quaid-i-Azam University Campus, Islamabad Pakistan
Microanalysis in Science and Engineering - Electron Microscopy A Workshop for Middle and High School Teachers sponsored by Tennessee Technological University.
Centre de Toulouse Radiation interaction with matter 1.
1 Semiconductor Detectors  It may be that when this class is taught 10 years on, we may only study semiconductor detectors  In general, silicon provides.
Ch. 2 – Anatomy of the X-ray Machine
Nano-Materials Characterization Yoram Shapira, EE Nano-bio-electronics Growth and Processing Characterization and Analysis Design and Modeling.
EDS Energy Dispersive Spectroscopy
Scanning Electron Microscope (SEM)
Scanning Electron Microscope (SEM)
NANO 225 Micro/NanoFabrication Electron Microscopes 1.
Reminders for this week Homework #4 Due Wednesday (5/20) Lithography Lab Due Thursday (5/21) Quiz #3 on Thursday (5/21) – In Classroom –Covers Lithography,
CAMTECH 2011 Regi. High energy e - beam scans sample surface (Raster - line by line). Provides information about surface and near-surface atoms – topography.
Proximity Effect in Electron Beam Lithography
NANO 230 Micro/Nano Characterization
Scanning capacitance microscopy
Conventional SEM Specimen at high vacuum – requires sample fixation and dehydration or freezing. Charging is minimized by coating sample with metal or.
SEM- Schematic Overview. Electron Detection Tungsten Filament Electron Source.
08/03/09 SEM signal generation
SEM Scanning Electron Microscope
X Rays LO: Describe how electron beams produce X Rays Calculate the current in terms of rate of flow of electrons.
Questions/Problems on SEM microcharacterization Explain why Field Emission Gun (FEG) SEM is preferred in SEM? How is a contrast generated in an SEM? What.
Energie zu niedrigen Preisen durch lasergetriebene Kernfusion? Heinrich Hora University of New South Wales, Sydney, Australien.
Radiology Steps in radiation production Kilovoltage and voltage.
SARDAR PATEL INSTITUTE OF TECHNOLOGY E.NO : Guide By:- V.N.Thakkar.
PPAC Jonathan Olson University of Iowa Thesis Defense 8 April 2005.
Do it with electrons !. Microscopy Structure determines properties We have discussed crystal structure (x-ray diffraction) But consider now different.
SEM Imaging - Magnification and Deflection System
Scanning Electron Microscopy
Laboratory equipment Lecture (3).
Introduction to Scanning Electron Microscope by Sameer S
X-ray Production Sharif Qatarneh Medical Physics Division
NANO 230 Micro/NanoFabrication
positive beam of particles emerging from hole in cathode anode (+) positive beam of particles emerging from hole in cathode.
Intermediate and High Voltage Microscopy
TEM and SEM.
Do it with electrons !.
Semiconductor Detectors
SEM Imaging - Magnification and Deflection System
Unit 2 Particles and Waves Electric Fields and Movements of Charge
전자와 시편의 상호작용(비탄성산란) 2θ Incident Beam (Primary electron)
Scanning Electron Microscopy (SEM)
Thermionic Emission – Learning Outcomes
Computed Tomography (C.T)
Units – SI Units (1) David Bailey © Class Leading Ltd. 2013
Units – SI Units (4) David Bailey © Class Leading Ltd. 2013
Presentation transcript:

Hong Koh Yiin -CAMTEC Image from:

 Voltage difference between the filament (cathode) and the anode ◦ Accelerates the electron beam towards the anode. 2

 The minimum distance that can be separated as two distinguishable points in the SEM image. 3 SEM Resolution Test Medium (Al-W Dendrites)

4 Resolutio n (nm) Accelerating Voltage (kV) FE-SEM (S- 4800) Primary electron beam Secondary electrons Backscattered electrons X-rays

5 Secondary Electron Detector Secondary electron emission signal – more widely used in SEM

Energy of accelerated electron, E = eV = ½ mv 2 e = charge of electron V = accelerating voltage m = rest mass of electron v = velocity of electron 6

7

8 Penetration Depth, H = A V 1.67, μm z 0.89 ρ A= atomic weight, g mol -1 V= accelerating voltage, kV z= atomic number ρ= density, g cm -3 Penetration Depth α Interaction Volume

 Penetration depth/interaction volume is a direct function of energy Å SrS Si 15 kV 10 kV 5 kV

10 Accelerating Voltage High Low High Resolution Low Resolution Unclear surface structures More edge effect More beam damage More charge-up Clear surface structures Less edge effect Less beam damage Less charge-up

11

12

13 Accelerating Voltage High Low High Resolution Low Resolution Unclear surface structures More edge effect More beam damage More charge-up Clear surface structures Less edge effect Less beam damage Less charge-up

14

15 Accelerating Voltage High Low High Resolution Low Resolution Unclear surface structures More edge effect More beam damage More charge-up Clear surface structures Less edge effect Less beam damage Less charge-up

16

17 Accelerating Voltage High Low High Resolution Low Resolution Unclear surface structures More edge effect More beam damage More charge-up Clear surface structures Less edge effect Less beam damage Less charge-up

18

19 5 kV, 50000x2 kV, 50000x 300 V, 50000x 200nm

20